JPH033463B2 - - Google Patents
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- Publication number
- JPH033463B2 JPH033463B2 JP4886382A JP4886382A JPH033463B2 JP H033463 B2 JPH033463 B2 JP H033463B2 JP 4886382 A JP4886382 A JP 4886382A JP 4886382 A JP4886382 A JP 4886382A JP H033463 B2 JPH033463 B2 JP H033463B2
- Authority
- JP
- Japan
- Prior art keywords
- switch
- load
- switch element
- circuit
- capacitor
- 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
Links
- 239000003990 capacitor Substances 0.000 claims description 21
- 238000010586 diagram Methods 0.000 description 6
- 238000009499 grossing Methods 0.000 description 2
- 230000007704 transition Effects 0.000 description 2
- 230000005540 biological transmission Effects 0.000 description 1
- 230000006378 damage Effects 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005265 energy consumption Methods 0.000 description 1
- 239000004744 fabric Substances 0.000 description 1
- 230000001771 impaired effect Effects 0.000 description 1
- 238000000034 method Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02M—APPARATUS 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
- H02M3/00—Conversion of DC power input into DC power output
- H02M3/02—Conversion of DC power input into DC power output without intermediate conversion into AC
- H02M3/04—Conversion of DC power input into DC power output without intermediate conversion into AC by static converters
- H02M3/10—Conversion of DC power input into DC power output without intermediate conversion into AC by static converters using discharge tubes with control electrode or semiconductor devices with control electrode
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- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Dc-Dc Converters (AREA)
Description
【発明の詳細な説明】
〔発明の技術分野〕
この発明はスイツチにかかる電圧または流れる
電流波形が共振の弧になるスイツチ式電力増幅器
の電力制御回路に関するものである。
〔発明の技術的背景とその問題点〕
従来スイツチ式電力増幅器はチヨツパー方式に
みられるように入力電源電圧を直接スイツチし、
そのスイツチ幅を変えて負荷への電力量を変える
ものと、D級電力増幅器にみられるように外部回
路を追加して入力電源電圧を直接スイツチしない
回路を構成し、スイツチにかかる電圧または流れ
る電流を共振の弧になるようにし、負荷への電力
量の変化はもう一つのコンバータを入力側に用い
て行つている。前者のチヨツパー方式のスイツチ
損失はスイツチ周波数が増大するにつれてスイツ
チの遷移損失が増大し、その限界はスイツチ素子
のスイツチスピードによつて決まる。一方後者の
D級電力増幅器のスイツチ損失はスイツチ周波数
が増大してもスイツチの遷移損失は余り増大せず
高効率なスイツチングができる。反面共振の条件
が外部回路によつて決つているのでスイツチ幅、
スイツチ周期を変えても負荷への電力はスムース
に変わらない。そのためにこのD級電力増幅器の
ようなスイツチ回路の負荷への電力の調節は前後
にもう一つの可変電圧装置を設置する必要があ
る。
〔発明の目的〕
この発明は上記の点に鑑みなされたもので共振
波形を利用したスイツチ式電力増幅器であり、共
振波形を保ちながら負荷への電力を広範囲に変え
得るスイツチ式の電力増幅器の電力制御回路を提
供することを目的とするものである。
〔発明の概要〕
この発明では、電圧共振形シングルエンド・ス
イツチ回路に直列共振回路を介して負荷回路を接
続するスイツチ式電力増幅回路において直列共振
回路を、負荷回路を経由しないで直接閉じるスイ
ツチを、負荷回路の入力端子間に設けることによ
つて電圧共振を維持しながら負荷回路への電力の
制御をスムーズにできるようにしたものである。
〔発明の実施例〕
以下この発明を実施例により詳細に説明する。
第1図はこの発明の一実施例を示す回路構成図で
ある。1は入力直流電源であり、この両端に電流
平滑用チヨーク2を介してトランジスタあるいは
サイリスタ(GTOも含む)等のスイツチ素子3
を接続する。このスイツチ素子3にダンパーダイ
オード5と共振用コンデンサ5を並列につなぐ。
またこのスイツチ素子3に電力転送用コンデンサ
6およびインダクタンス7を介してスイツチ8を
接続する。このスイツチ8に並列に負荷回路9を
接続する。この負荷回路は単純に抵抗だけの場合
とブリツヂ整流器を経て電圧平滑コンデンサおよ
び負荷抵抗等を含む場合等も含む。
ここで第1図の動作を説明するために若干の仮
定をする。スイツチ素子3は一定のパルス幅およ
び周期で開閉し、第1図の回路は定常状態に達し
ているとする。すなわちチヨーク2には一定電流
Iinが流れ、周期開始時における共振用コンデン
サ6の端子電圧はある一定値Vc1なつていて、更
に電力伝送用インダクタンス7にも電流がある一
定値Ioだけ流れているとする。スイツチ素子3,
8およびダイオード5はそれぞれ理想スイツチと
し、導通時には伝導抵抗は零オーム、断時には無
限大である。
先づ簡単のたゆスイツチ素子8は開きつばなし
の状態で、スイツチ素子3が“導通”の状態の期
間から本発明の動作を説明する。
第1図において負荷回路9を具体的に抵抗11
で表わして、スイツチ素子3が“導通”のとき等
価回路は第2図のようになる。そして文献N.O.
Sokal“clossE−Arka closs of High−
Efficiency Twad Sigle−Euded Switching
Power Awplifier”IEEE Vol SC−10No.3
June1975によるとあらかじめ負荷抵抗11の値
Rをスイツチの動作周波数とインダクタンス7
の値Lとを用いておおよそ
2π・L/RL>6 …(1)
程度に選択しておく。
チヨーク2には電源1から電流が流れ込んで磁
気エネルギーの補給を行う。一方負荷11を一部
に含む閉路においてはインダクタンス7に蓄積さ
れていた磁気エネルギーを電流Loutとして図示
の方向に流して放出する。その間Loutは負荷RL
にエネルギーを消費しながら、コンデンサ6にエ
ネルギーを電圧の形で蓄積する。この状態は動作
周期の半分まで継続する。すなわち動作周期の半
分の経過後スイツチ素子3は強制的に“断”状態
になる。そのとき、電源1とチヨークコイル2は
一定電流Loutを供給する電流源となり、スイツ
チ素子3両端に接続されていたコンデンサ4が表
われるのでスイツチ素子3の“断”の期間の等価
回路は第3図のようになる。
コンデンサ4には電流源12からの流入と、共
振回路10に蓄積されていたエネルギーの流入が
ある。そしてコンデンサ4,6とコイル7および
負荷11で共振回路を形成するために、コンデン
サ4の端子電圧は正弦波の弧を描いて上昇し再び
降下してやがて零になり更に負電位になろうとす
る。そのときコンデンサ4の両端にダイオード5
が第1図に示す向きに入つているために等価回路
は再び第2図に戻る。すなわち動作周期が終るま
でコンデンサ4の端子電圧は零に保たれている。
その後次の周期が始まるとスイツチ素子3の端子
電圧は零の状態で電流が流れ始めるのでスイツチ
素子3の投入時のスイツチ損失は原理的になくな
る。以上の動作波形をまとめると第4図のように
なる。すなわち第4図aはスイツチ素子3の“導
通”,“断”の配分を示し、bはスイツチ素子3の
電流波形を、cはスイツチ素子3の端子電圧波形
を、dは負荷RLに流れる電流波形をそれぞれ示
した。但し第3図の負荷電流Loutの実線の向き
は第4図のdの負の部分が対応する。
ここで負荷RLが変動しても(1)式を満たす範囲
に入つているときには第4図の各部波形は大幅に
変わることはないが負荷RLが軽くなり(1)式の範
囲を出ると負荷電流Loutの減衰が第4図dの点
線に示すように激しくなりスイツチ素子3が
“断”になつたとき共振回路10に蓄積されてい
たエネルギーが少ないのでコンデンサ4の電圧が
第4図cの点線で示すように一周期が終了しても
電位が零にならない。すなわちコンデンサ4に電
圧Vresを残したまま次の周期が始まると1/2
CV2resだけの電気エネルギーがスイツチ素子3
に一瞬の内に流れる。そのことは第4図bの点線
に示すようにスパイク状の大きな電流となる。そ
の結果スイツチ素子3は許容電流値を起え破壊す
る。また破壊に至らない場合はスイツチ素子での
損失が著しく増大する。
以上の事実から負荷を軽い方向に変えるにはコ
ンデンサ4の端子電圧Vcが零になれるエネルギ
ーが、スイツチ素子の“導通”期間に共振回路1
0に蓄えられていないといけないことになる。こ
のことを言い換えると共振回路10に端子電圧
Vcを零にできるエネルギーが蓄えられているの
が負荷RLを軽るくできる限界になる。その負荷
の可変範囲は狭く定格負荷RLから1/5倍程度で各
部波形が第4図の点線のようになる。
この負荷の可変範囲の狭くなる原因は共振回路
10に、コンデンサ4の端子電圧を零まで下げる
のに十分なエネルギーが蓄められないことにある
かまたは端子電圧Vcを零まで下げるのに十分な
エネルギーが蓄まつているにもかかわらず負荷
RLでエネルギー消費が大きいために共振回路1
0の蓄積エネルギーがコンデンサ4に伝わらない
ことにある場合の二通りである。この後半の状態
は本発明によれば救済できる。すなわち負荷RL
の両端にスイツチを設けて負電流Loutを適当な
時期Taに閉じて共振回路10のエネルギーを負
荷RLを経由しないで直接コンデンサ4に伝える
ようにすれば端子電圧Vcは零になる。
スイツチ8のON−OFFチヤートは一周期Tの
中で第5図eに示すようにTonの中で一回とTon
〜Tまでの中で一回それぞれ閉じる。スイツチ8
が開いている時期Taは第4図において各部波形
は点線部分になり、閉じている期間(Ton−Ta)
は第4図の実線部分になるのでそれらスイツチ8
のON−OFFチヤートに従つて書ひ直すと各部波
形は第5図b〜dになる。すなわちスイツチ素子
3に流れる波形はb図に、スイツチ素子3にかか
る波形はc図に共振回路10に流れる電流波形は
dにそれぞれ示した。
ここでTa経過後スイツチ8で切り換えられ共
振回路10の大きな共振電流がコンデンサ4に流
れ込むので端子電圧Vcの振幅は第5図bに示す
ように大きく振動し一周期が終了する時刻には零
になる。
スイツチ8が閉じている期間(Ton−Ta),
(T−Ta)は負荷11には電力は伝わつてないの
で負荷11の平均電力は減少する。またTaの幅
を変えれば負荷11で消費される平均電力は任意
に変えられる。
スイツチ8はサイリスタを第6図に示すように
逆平行に接続しても良いしトランジスタ等又は磁
気増幅器等でも直接第5図eに示すスイツチのチ
ヤートに従つてスイツチすれば容易に実現でき
る。
〔発明の効果〕
以上の説明から明らかなように主スイツチ3が
スイツチ損失の少ない動作をしているのにもかか
わらず補助スイツチ8の導通時期を変えることに
よつて負荷11への消費電力をスムース変えるこ
とができる。
また負荷回路9中の中身は第7図に示すものを
用いても基本動作はそこなわれない。しかも負荷
抵抗11の端子電圧は補助スイツチ8が閉じても
零になることはない。 DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a power control circuit for a switch type power amplifier in which the voltage applied to a switch or the current waveform flowing through the switch becomes an arc of resonance. [Technical background of the invention and its problems] Conventional switch type power amplifiers directly switch the input power supply voltage as seen in the chopper type.
There are two types of circuits: those that change the width of the switch to change the amount of power sent to the load, and those that do not directly switch the input power supply voltage by adding an external circuit as seen in class D power amplifiers. is made to form a resonant arc, and the amount of power to the load is changed using another converter on the input side. In the former chopper type switch loss, the transition loss of the switch increases as the switch frequency increases, and its limit is determined by the switch speed of the switch element. On the other hand, regarding the switch loss of the latter class D power amplifier, even if the switch frequency increases, the transition loss of the switch does not increase much, allowing highly efficient switching. On the other hand, since the resonance conditions are determined by the external circuit, the switch width,
Even if the switch cycle is changed, the power to the load does not change smoothly. Therefore, in order to adjust the power to the load of a switch circuit such as this class D power amplifier, it is necessary to install another variable voltage device before and after the switch circuit. [Object of the Invention] This invention was made in view of the above points, and is a switch-type power amplifier that utilizes a resonant waveform. The purpose is to provide a control circuit. [Summary of the Invention] The present invention provides a switch type power amplifier circuit in which a load circuit is connected to a voltage resonant single-ended switch circuit via a series resonant circuit, and a switch that directly closes the series resonant circuit without going through the load circuit. By providing this between the input terminals of the load circuit, it is possible to smoothly control the power to the load circuit while maintaining voltage resonance. [Examples of the Invention] The present invention will be described in detail below with reference to Examples.
FIG. 1 is a circuit diagram showing an embodiment of the present invention. 1 is an input DC power supply, and a switch element 3 such as a transistor or thyristor (including GTO) is connected to both ends of the input DC power supply via a current smoothing chain 2.
Connect. A damper diode 5 and a resonance capacitor 5 are connected in parallel to this switch element 3.
Further, a switch 8 is connected to this switch element 3 via a power transfer capacitor 6 and an inductance 7. A load circuit 9 is connected in parallel to this switch 8. This load circuit includes cases in which it simply includes only a resistor, and cases in which it includes a voltage smoothing capacitor, load resistance, etc. via a bridge rectifier. Here, some assumptions will be made to explain the operation of FIG. It is assumed that the switch element 3 opens and closes with a constant pulse width and period, and the circuit shown in FIG. 1 has reached a steady state. In other words, a constant current is applied to the chain 2.
It is assumed that Iin flows, the terminal voltage of the resonant capacitor 6 at the start of the cycle is a certain constant value Vc1 , and furthermore, a certain constant value Io of current flows in the power transmission inductance 7. switch element 3,
8 and diode 5 are each ideal switches, and the conduction resistance is zero ohm when conductive, and infinite when disconnected. First, the operation of the present invention will be explained from the period when the switch element 3 is in the "conducting" state with the simple switch element 8 in an open state without a collar. In FIG. 1, the load circuit 9 is specifically represented by a resistor 11.
When the switch element 3 is "conductive", the equivalent circuit becomes as shown in FIG. And literature no.
Sokal“clossE−Arka cloth of High−
Efficiency Twad Sigle−Euded Switching
Power Awplifier”IEEE Vol SC−10No.3
According to June 1975, the value R of the load resistance 11 is determined in advance by the operating frequency of the switch and the inductance 7.
Using the value L, select approximately 2π·L/R L > 6 (1). Current flows into the chain 2 from the power source 1 to replenish magnetic energy. On the other hand, in a closed circuit including the load 11 as a part, the magnetic energy stored in the inductance 7 is discharged by flowing in the direction shown in the figure as a current Lout. Meanwhile, Lout is the load R L
While consuming energy, energy is stored in the capacitor 6 in the form of voltage. This state continues until half of the operating cycle. That is, after half of the operating cycle has elapsed, the switch element 3 is forcibly turned off. At that time, the power supply 1 and the switch coil 2 become a current source that supplies a constant current Lout, and the capacitor 4 connected to both ends of the switch element 3 appears, so the equivalent circuit during the "off" period of the switch element 3 is shown in Figure 3. become that way. The capacitor 4 receives an inflow from a current source 12 and an inflow of energy stored in the resonant circuit 10 . Since the capacitors 4 and 6, the coil 7, and the load 11 form a resonant circuit, the terminal voltage of the capacitor 4 rises in a sinusoidal arc, drops again, and eventually reaches zero, becoming even more negative potential. . At that time, a diode 5 is connected across the capacitor 4.
is in the direction shown in FIG. 1, the equivalent circuit returns to FIG. 2 again. That is, the terminal voltage of the capacitor 4 is maintained at zero until the end of the operating cycle.
Thereafter, when the next cycle begins, current begins to flow with the terminal voltage of the switch element 3 being zero, so that the switch loss when the switch element 3 is turned on is theoretically eliminated. The above operation waveforms are summarized as shown in FIG. In other words, Fig. 4a shows the distribution of "conduction" and "disconnection" of the switch element 3, b shows the current waveform of the switch element 3, c shows the terminal voltage waveform of the switch element 3, and d flows to the load R L. The current waveforms are shown respectively. However, the direction of the solid line of the load current Lout in FIG. 3 corresponds to the negative part of d in FIG. 4. Here, even if the load R L changes, if it is within the range that satisfies equation (1), the waveforms of each part in Figure 4 will not change significantly, but the load R L will become lighter and go out of the range of equation (1). When the load current Lout attenuates rapidly as shown by the dotted line in Fig. 4d, and the switch element 3 becomes disconnected, there is little energy stored in the resonant circuit 10 , so the voltage across the capacitor 4 increases as shown in Fig. 4. As shown by the dotted line c, the potential does not become zero even after one cycle ends. In other words, when the next cycle starts with the voltage Vres remaining in the capacitor 4, the electrical energy of 1/2 CV 2 res is transferred to the switch element 3.
It flows in an instant. This results in a large spike-like current as shown by the dotted line in FIG. 4b. As a result, the switch element 3 increases its allowable current value and is destroyed. Furthermore, if destruction does not occur, the loss in the switch element increases significantly. From the above facts, in order to change the load to a lighter direction, the energy needed to make the terminal voltage Vc of the capacitor 4 zero is required to reduce the load to the resonant circuit 1 during the "conduction" period of the switch element.
This means that it must be stored at 0. In other words, the terminal voltage is applied to the resonant circuit 10 .
The limit to which the load R L can be lightened is that the energy that can reduce Vc to zero is stored. The variable range of the load is narrow, about 1/5 times the rated load R L , and the waveforms at various parts become as shown by the dotted lines in Figure 4. The cause of this narrowing of the variable range of the load is that sufficient energy is not stored in the resonant circuit 10 to reduce the terminal voltage of the capacitor 4 to zero, or that sufficient energy is not stored in the resonant circuit 10 to reduce the terminal voltage Vc to zero. Load despite stored energy
Resonant circuit 1 due to large energy consumption in R L
There are two cases where the stored energy of 0 is not transmitted to the capacitor 4. This latter state can be relieved according to the present invention. i.e. load R L
If a switch is provided at both ends of , the negative current Lout is closed at an appropriate time Ta, and the energy of the resonant circuit 10 is transmitted directly to the capacitor 4 without passing through the load R L , the terminal voltage Vc becomes zero. The ON-OFF chart of switch 8 is once in Ton and once in Ton in one period T, as shown in Figure 5e.
Close each once between ~T. switch 8
In Fig. 4, the period Ta when Ton is open is indicated by the dotted line, and the period Ta is closed is (Ton-Ta)
is the solid line part in Figure 4, so those switches 8
When rewritten according to the ON-OFF chart, the waveforms of each part become as shown in Figures b to d. That is, the waveform flowing through the switch element 3 is shown in figure b, the waveform applied to the switch element 3 is shown in figure c, and the waveform of the current flowing in the resonant circuit 10 is shown in figure d. After Ta has elapsed, the switch 8 is switched and a large resonant current of the resonant circuit 10 flows into the capacitor 4, so the amplitude of the terminal voltage Vc oscillates greatly as shown in Figure 5b and becomes zero at the end of one cycle. Become. The period during which switch 8 is closed (Ton-Ta),
(T-Ta), since no power is transmitted to the load 11, the average power of the load 11 decreases. Furthermore, by changing the width of Ta, the average power consumed by the load 11 can be changed arbitrarily. The switch 8 can be easily realized by connecting thyristors in antiparallel as shown in FIG. 6, or by directly switching a transistor or a magnetic amplifier according to the switch chart shown in FIG. 5e. [Effects of the Invention] As is clear from the above explanation, even though the main switch 3 operates with low switch loss, the power consumption of the load 11 can be reduced by changing the conduction timing of the auxiliary switch 8. Can be changed smoothly. Furthermore, even if the contents of the load circuit 9 shown in FIG. 7 are used, the basic operation will not be impaired. Furthermore, the terminal voltage of the load resistor 11 does not become zero even when the auxiliary switch 8 is closed.
第1図はこの発明の一実施例を示す回路構成
図、第2図および第3図は動作を説明するための
等価回路図、第4図および第5図は動作波形図、
第6図はスイツチの構成法を示す図、第7図は負
荷回路の一例を示す図である。
1…電源、2…チヨーク、3,8…スイツチ素
子、4,6,13,…コンデンサ、7…インダク
タンス、9…負荷回路、10…共振回路、11…
負荷抵抗、12…電流源、14…ブリツジダイオ
ード。
FIG. 1 is a circuit configuration diagram showing an embodiment of the present invention, FIGS. 2 and 3 are equivalent circuit diagrams for explaining the operation, and FIGS. 4 and 5 are operational waveform diagrams.
FIG. 6 is a diagram showing a method of configuring the switch, and FIG. 7 is a diagram showing an example of a load circuit. DESCRIPTION OF SYMBOLS 1... Power supply, 2... Chain yoke, 3, 8... Switch element, 4, 6, 13,... Capacitor, 7... Inductance, 9... Load circuit, 10 ... Resonant circuit, 11...
Load resistance, 12... Current source, 14... Bridge diode.
Claims (1)
するスイツチ素子を接続し、このスイツチ素子に
並列にコンデツサとダンパーダイオードを接続
し、このスイツチ素子に他のコンデンサを介して
コイルを介し負荷回路を接続し、この負荷回路に
並列に他のスイツチ素子を接続したことを特徴と
する電力制御回路。 2 負荷回路に並列に接続したスイツチ素子は少
なくとも、チヨークを介して接続したスイツチ素
子が“導通”時に1回,“断”時に1回それぞれ
開閉するスイツチ作動をすることを特徴とする特
許請求の範囲第1項記載の電力制御回路。[Claims] 1. A switch element that opens and closes under certain conditions is connected to a DC power supply via a chain yoke, a capacitor and a damper diode are connected in parallel to this switch element, and a coil is connected to this switch element via another capacitor. 1. A power control circuit characterized in that a load circuit is connected through the circuit, and another switch element is connected in parallel to the load circuit. 2. A patent claim characterized in that the switch element connected in parallel to the load circuit operates at least once when the switch element connected via the chain yoke opens and closes once when it is "conducted" and once when it is "disconnected". The power control circuit according to scope 1.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4886382A JPS58170358A (en) | 1982-03-29 | 1982-03-29 | Electric power control circuit |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4886382A JPS58170358A (en) | 1982-03-29 | 1982-03-29 | Electric power control circuit |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58170358A JPS58170358A (en) | 1983-10-06 |
| JPH033463B2 true JPH033463B2 (en) | 1991-01-18 |
Family
ID=12815110
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4886382A Granted JPS58170358A (en) | 1982-03-29 | 1982-03-29 | Electric power control circuit |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58170358A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4945466A (en) * | 1989-02-22 | 1990-07-31 | Borland Walter G | Resonant switching converter |
| US5164891A (en) * | 1991-08-21 | 1992-11-17 | Power Integrations, Inc. | Low noise voltage regulator and method using a gated single ended oscillator |
-
1982
- 1982-03-29 JP JP4886382A patent/JPS58170358A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58170358A (en) | 1983-10-06 |
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