JPS5872345A - Charing and discharging power source - Google Patents
Charing and discharging power sourceInfo
- Publication number
- JPS5872345A JPS5872345A JP56168974A JP16897481A JPS5872345A JP S5872345 A JPS5872345 A JP S5872345A JP 56168974 A JP56168974 A JP 56168974A JP 16897481 A JP16897481 A JP 16897481A JP S5872345 A JPS5872345 A JP S5872345A
- Authority
- JP
- Japan
- Prior art keywords
- charging
- discharging
- section
- phase
- cycle
- 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
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Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
(1) 発明の分野
本発明は充放電部の段数変化に対し効率的かつ正確に充
電を行ないよって放電の安定度を向上させた充放電用電
源装置に関する。DETAILED DESCRIPTION OF THE INVENTION (1) Field of the Invention The present invention relates to a charging/discharging power supply device that improves the stability of discharging by efficiently and accurately charging even when the number of stages in a charging/discharging section changes.
(2) 従来技術
■、一般に、簡単にパルスを得る装置としては、電源部
と充放電用コンデンサとで構成し、充放電コンデンサの
充電、放電によってパルスを得るようにしている0%に
この株の装置1U、レーザー光を得る場合の光励起用装
置として広く用いられている。ところでレーザーは近来
、溶接、切断、溝切シ等の加工分野ではその用途も広い
。(2) Prior art■ Generally, as a device for easily obtaining pulses, this type of device consists of a power supply section and a charging/discharging capacitor, and obtains pulses by charging and discharging the charging/discharging capacitor. The device 1U is widely used as a device for optical excitation when obtaining laser light. By the way, lasers have recently been widely used in processing fields such as welding, cutting, and grooving.
したがって各加工用途に応じた照射エネルギーや照射時
間をもったレーザー光が必賛となり、その手段として従
来、前記の充放電コンデンサの充tt圧や使用段数を変
え、各用途に応じたレーザー光を得ている。つまり照射
時間の長いレーザー光を得るには、充放電コンデンサの
使用段数を増やしその放電時間を長くして、光励起時間
を長くし、照射時間を短かくするには充放電コンデンサ
の使用段数を減らし、光励起時間を短かくすれば良いの
である。この場合充放電コンデンサの放電時は充放電コ
ンデンサへの電源部からの充wは停止される様罠なって
いる。Therefore, a laser beam with irradiation energy and irradiation time suitable for each processing application is indispensable, and as a means to achieve this, conventionally, the charging/discharging capacitor's charging/discharging capacitor's charging tt pressure and the number of stages used have been changed, and laser light according to each application has been used. It has gained. In other words, in order to obtain a laser beam with a long irradiation time, the number of stages of charge/discharge capacitors used is increased and the discharge time is lengthened, and the photoexcitation time is lengthened.To shorten the irradiation time, the number of stages of charge/discharge capacitors used is reduced. , the optical excitation time can be shortened. In this case, when the charging/discharging capacitor is discharging, charging from the power supply unit to the charging/discharging capacitor is stopped.
■、また充電を行なうに際し、50/60Hzの商用周
波数を用いて充電電源とした場合、交流位相制御回路を
用いて充t%流と充電電圧をフィードバックしながら充
電を行なうものや、商用電源を直流に変換し、これを高
い周波数のDC−DCコンバータによりて直流充電を行
なったりするものがある。■Also, when charging, if a commercial frequency of 50/60Hz is used as a charging power source, there are those that use an AC phase control circuit to feed back the charging % flow and charging voltage, and those that use a commercial power source. There is a method that converts it into direct current and performs direct current charging using a high frequency DC-DC converter.
(3)従来技術の問題点
前記■の従来技術にては充放電コンデンサの使用段数を
大幅に変えた場合電源部よシの充電時間が大幅に変化し
、こねに対応を取らせるための充電制御1は非常に困難
であった。したがって充電の精度か悪くなシ、よって放
電の安定度も悪くなって所望のレーザー光を得られない
欠点を根本的にもりている。(3) Problems with the conventional technology In the conventional technology described in (■) above, when the number of stages of charging/discharging capacitors used is significantly changed, the charging time of the power supply section changes significantly, and the charging time required to respond to the kneading process is Control 1 was very difficult. Therefore, the accuracy of charging is poor, and the stability of discharging is also poor, resulting in a fundamental drawback that the desired laser light cannot be obtained.
また前記■においては前記の根本的欠点を考慮したもの
であるが、フィードバックの時間遅レニヨる制御回路の
不安定さのため放電コンデンサの大容量時および小容量
時での過大−流および過充電Fiまぬかれなく、充電の
精度を上げることが困難である。さらにDC−DCコン
バータの使用においては回i8が複雑となシ製作上好ま
しくない。In addition, although the above-mentioned fundamental drawback is taken into consideration in the above-mentioned item (2), due to the instability of the control circuit due to the feedback time delay, excessive current and overcharging occur when the discharge capacitor has a large capacity or a small capacity. It is difficult to improve charging accuracy without impairing Fi. Furthermore, when using a DC-DC converter, the circuit i8 is complicated, which is not preferable in terms of manufacturing.
(4)発明の目的
本発明は充放電部の容i変化に対しても均一な高い精度
で充電が行なえよって安定な放電状llを得られる製作
上簡羊な充放覧用ItIL源装置を提供することにある
。(4) Purpose of the Invention The present invention provides an ItIL source device for charging/discharging that is easy to manufacture and can perform charging uniformly and with high precision even when the capacity i of the charging/discharging section changes, thereby obtaining a stable discharge condition. It is about providing.
(5)発明の要点
本発明は充放電部の充電を行なうに際し、充電を所定の
充電サイクルで行ない、各充電サイクルでの充電電圧を
逐次検出し比較増幅M Kて基準電圧と比較し、その比
較信号に応じて各充電サイクルでの充放電部への通覧位
相を制御して/’/T定の充11L電圧に充電するもの
であ゛る。また充放電部の容量を変えた場合は、前記通
電位相の初期通電位相をその容量に応じた値に設定する
ことによ)上記目的を達成するものである。(5) Key Points of the Invention The present invention, when charging a charging/discharging section, performs charging in a predetermined charging cycle, sequentially detects the charging voltage in each charging cycle, and compares it with a reference voltage using comparison amplification MK. The phase of communication to the charging/discharging section in each charging cycle is controlled in accordance with the comparison signal, and charging is performed to a constant charging voltage of /'/T. Furthermore, when the capacity of the charging/discharging section is changed, the above object is achieved by setting the initial energization phase of the energization phase to a value corresponding to the capacity.
(6)発明の夾施例 −
次に本発明の一実施例″を′第1図、第2図および第3
図を用いて&明する。なお、第1図は構成図を、第2図
および第3図は特性図を示す。(6) Additional Embodiments of the Invention - Next, an embodiment of the present invention is shown in Figures 1, 2, and 3.
Explain & explain using diagrams. Note that FIG. 1 shows a configuration diagram, and FIGS. 2 and 3 show characteristic diagrams.
端子Uと端子■および端子Uと端子wFi交”流電源端
子で、端子U−W’間にはラッ゛シ&電流防止用コイル
1と、極性を逆にして′並列′接続した制御整流素子2
,3(す1イリス゛りな′ど)と、電源トランス4の一
次側とが直列に接続されている。Terminals U and Terminal ■ and Terminal U and Terminal wFi are AC power terminals, and between terminals U and W' there is a lash and current prevention coil 1, and a control rectifier connected in 'parallel' with the polarity reversed. 2
, 3 (such as 1 iris) and the primary side of the power transformer 4 are connected in series.
また前記端子U’−V間には移相トランス5の′−一次
側接続されている。かかる端子U−V間の交流周波数に
基づき充電サイクルが決まる。そして前記tL休体ラン
スイの二次側には整流回路6が接続さね、この整流回路
6の田力両端には光放電用コンデンサ7.8と、抵抗9
および10の直列回路と、放電発光する放電管11とが
それぞれ相互並列に接続されている。なお前記充放電用
コンデン?7はスイッチS1を介して整流回路6と接続
される様になっている。さらに前記放電管11の近傍に
は開放電管11からのノ臂ルス光を受けて光励起される
レーザー物質12が設置されこのレーザー物質12の光
軸上に同レーザー物質12の光を反射する置方が半鏡藺
、他方が鏡面の一対の共振ミラー13が前記レーザー物
質12°を介して向かい合う様に設置されている。まf
c14は所定の基準を圧と充電電圧を比較する比較増幅
回路で、この比較増幅回路14の入力端の負側端には前
記抵抗9と10の共通接続部が接続され、上側端には直
流電源15.より抵抗16を介して印加される基準電圧
調整用抵抗17の摺動部が接続されている。さらにこの
基準電圧調整用抵抗17の両端には調整用抵抗17の印
加電圧を短絡するスイッチSLが接続されている。そし
て前記比較増幅回路14の出力側に比較増幅回路14の
信号に応じて11流制−をするトランジスタ18のペー
ス側か接続されている。Further, the '-primary side of the phase shift transformer 5 is connected between the terminals U' and V. The charging cycle is determined based on the AC frequency between the terminals UV. A rectifier circuit 6 is connected to the secondary side of the tL rest body run, and a photodischarge capacitor 7.8 and a resistor 9 are connected to both ends of the rectifier circuit 6.
and 10 series circuits and discharge tubes 11 that discharge and emit light are connected in parallel with each other. What about the charge/discharge capacitor mentioned above? 7 is connected to a rectifier circuit 6 via a switch S1. Further, near the discharge tube 11, a laser material 12 that is optically excited by receiving the nostril light from the open tube 11 is installed, and a device that reflects the light of the laser material 12 is placed on the optical axis of the laser material 12. A pair of resonant mirrors 13, one half-mirror and the other mirror, are installed so as to face each other with the laser material 12 degrees in between. Maf
C14 is a comparison amplifier circuit that compares the charging voltage with a predetermined reference voltage.The negative input terminal of this comparison amplifier circuit 14 is connected to the common connection of the resistors 9 and 10, and the upper end is connected to the DC voltage. Power supply 15. A sliding portion of a reference voltage adjusting resistor 17 applied via a resistor 16 is connected thereto. Furthermore, a switch SL for short-circuiting the voltage applied to the adjustment resistor 17 is connected to both ends of the reference voltage adjustment resistor 17. The output side of the comparison amplifier circuit 14 is connected to the pace side of a transistor 18 which controls 11 currents according to the signal from the comparison amplifier circuit 14.
一方、mj記移相トランス5の二次側の一端には移相用
コンデンサ19が接続されこの出力側と移相トランス5
の二次側のもう一端の間にはダイオード20,21.2
2.23によって形成されたプリツー/整流回路の入力
端が接続されている。On the other hand, a phase-shifting capacitor 19 is connected to one end of the secondary side of the phase-shifting transformer 5 mj, and the output side and the phase-shifting transformer 5 are connected to each other.
A diode 20, 21.2 is connected between the other ends of the secondary side of the
The input end of the pre-two/rectifier circuit formed by 2.23 is connected.
さらにこのブリッジlI流回路の出力側の一端は抵抗2
4を介して前記トランジスタ18のコレクタ側に接続さ
ね、もう−錫はエミッタ側に接続さhている。なお、前
記抵抗24に祉抵抗25がスイッチSlを介して並列に
*aされる様になっており、またスイッチSS と前記
スイッチS1とは連動さねている。また、移相トランス
5の二次側の中点と前記移相用コンデンサ19の出力側
との間の電圧差によってダートパルスを出力するダート
パルス発生回路26が移相トラフ1502次側中点およ
び移相用コンデンサ19の出力側に接続されている。そ
してこのゲートパルス発生回路26の出力によって前記
制御整流素子2,3は動作を行なう様になっている。Furthermore, one end of the output side of this bridge II current circuit has a resistor 2
4 is connected to the collector side of the transistor 18, and tin is connected to the emitter side of the transistor 18. Note that a resistor 25 is connected in parallel to the resistor 24 via a switch Sl, and the switch SS and the switch S1 are not interlocked. Further, a dirt pulse generation circuit 26 that outputs a dirt pulse by a voltage difference between the middle point of the secondary side of the phase shifting transformer 5 and the output side of the phase shifting capacitor 19 is connected to the middle point of the secondary side of the phase shifting trough 150 and It is connected to the output side of the phase shifting capacitor 19. The control rectifying elements 2 and 3 operate according to the output of the gate pulse generating circuit 26.
また、zvFi*ラッシーランプ11の放電開始用のク
ロ・ツク発振回路で、このクロック発振回路27にFi
創記スイッチS−の開閉を行なう開閉回路28が接続さ
れ、この開閉回路28にはフラッジエランプ11に外巻
されたトリガ電極29管介してフラッジエランfilに
起動用トリガを与えるトリガ回路30が接続されている
。In addition, in the clock oscillation circuit for starting discharge of the zvFi* Lassi lamp 11, this clock oscillation circuit 27 is connected to Fi.
An opening/closing circuit 28 is connected to open and close the creation switch S-, and a trigger circuit 30 is connected to this opening/closing circuit 28 to provide a starting trigger to the Fludge Elan fil through a trigger electrode 29 tube wound around the Fludge Elamp 11. has been done.
次に、以上の様に構成された装置の説明をすると、まず
パルス幅の広いノ臂ルス波形を発生させる場合には、前
記スイッチS1および5sri閉じられている。この状
態で充電を行なう場合、前記クロック発振回路27から
クロック信号に出力されず、シタがってスイッチSsU
開状態にある。そして端子UVおよび端子UW間に交流
が印加されると、前記比較増幅回路14の正 □側端
には前記直流電源15によって設定された基準1圧が入
力される。したかつてこの比較増幅回路14の出力には
正信号が出力され前記トランジスタ18を完全オン状態
にする。すなわち前記移相トラン≠スt5の二次側回路
はトランジスタ18を介して閉回路が形成され主に前記
移相コンデンサ19の容量と前記抵抗24および25の
並列抵抗分との時定数に基づいた信号が移相トランス5
の二次側中点と移相コンデンサ19の出力側間に生じる
。この2点間の信号が前記)f −) /4’ルス発生
回路26に入力される。そしてこのグートノ母ルス発生
回路26は第2図にボすθlの導通角で削整制御整流素
子2゜3を制御する。以上によシ1サイクルにおいて、
前記電源トランス4の一次@あるいは二次側には第2図
の1の様な電圧波形あるいはbの様な電流整形が得られ
る。なお、正弦波UWは端子U−W間の電源波形である
。このようにして得られた電圧あるいに電流Fi削削整
移相トランスの二次側の整流回路6によって全波整流さ
れ前記充放電コンデンサ7.8に充電される0以上によ
シ充電され比電圧は前記抵抗9,10の接続点より前記
比較増幅回路14の負側端にフィードバックされ、前記
と同様に正側端の基準電圧と比較される。この時負側ル
寛圧と正側端気圧との差は前記充電サイクルの時より減
少している。そのため比較増幅回路14の出力は減少し
、前記トランジスタ18はコレクタ電流を減少する。し
たがって前記移相トランス5の二次側の時定数は主に前
記移相コンデンサ9、抵抗24と25の並列分、さらに
トランジスタ18のコレクタ電流の減少によって生じた
抵抗分で素子2,3の導通角は減少する。すなわち前記
充放電コンデンサr、ttへの充電量は減少する。Next, the apparatus constructed as above will be explained. First, when generating a knee pulse waveform with a wide pulse width, the switches S1 and 5sri are closed. When charging is performed in this state, the clock signal is not output from the clock oscillation circuit 27, and the switch SsU is shifted.
It is in the open state. When an alternating current is applied between the terminals UV and UW, the reference voltage of 1 set by the direct current power supply 15 is input to the positive side end of the comparison amplifier circuit 14. Once this happens, a positive signal is output from the comparison amplifier circuit 14, turning the transistor 18 completely on. That is, the secondary side circuit of the phase shift transformer ≠ t5 is formed as a closed circuit via the transistor 18, and is mainly based on the time constant of the capacitance of the phase shift capacitor 19 and the parallel resistance of the resistors 24 and 25. Signal phase shift transformer 5
occurs between the middle point of the secondary side of the phase shift capacitor 19 and the output side of the phase shift capacitor 19. The signal between these two points is input to the )f-)/4' pulse generating circuit 26. The goutton pulse generating circuit 26 controls the cutting control rectifying element 2.degree. 3 at the conduction angle .theta.l shown in FIG. In one cycle above,
On the primary or secondary side of the power transformer 4, a voltage waveform as shown in 1 in FIG. 2 or a current shaping as shown in b in FIG. 2 can be obtained. Note that the sine wave UW is a power waveform between terminals UW. The voltage or current Fi obtained in this way is full-wave rectified by the rectifier circuit 6 on the secondary side of the cutting phase shift transformer, and is charged by 0 or more to be charged to the charge/discharge capacitor 7.8. The specific voltage is fed back to the negative end of the comparison amplifier circuit 14 from the connection point between the resistors 9 and 10, and is compared with the reference voltage at the positive end in the same manner as described above. At this time, the difference between the negative end pressure and the positive end pressure is smaller than in the charging cycle. Therefore, the output of the comparison amplifier circuit 14 decreases, and the transistor 18 decreases its collector current. Therefore, the time constant on the secondary side of the phase shift transformer 5 is mainly due to the parallel component of the phase shift capacitor 9, the resistors 24 and 25, and the resistance generated by the decrease in the collector current of the transistor 18, which makes the elements 2 and 3 conductive. The angle decreases. That is, the amount of charge to the charging/discharging capacitors r and tt decreases.
以上のような作用の〈シ返しにより所定の電圧までの充
電が行なわれる。なお、このくり返し周期は前記端子U
−4間の交流電源周波数に起因するものである6以上こ
のくり返し過程の充電電圧および充電電流を第3図の実
線■lお上び実線!1−4〜■1−4に示す、なお、■
。は所定電圧を、ts=tsti時刻を示しt!〜tl
;tl〜tl 、・・・+t@”−t@の各−jは
等時間で前記制御整流素子2,3の導通01サイクル時
間に相当する。また縦軸■は充電電流を、pH放電電流
を示し、各充電サイクルでの電流!、−1〜■、−4の
波高値が異なるのは充電が進むにつれて前記トランジス
タ18の電流が減少し、充放電コンデンサ7.8の充電
量が各サイクルで逐次増加して、前記導通角θ宜か小さ
くなるからである。Charging to a predetermined voltage is performed by reversing the above-described actions. Note that this repetition period is the same as that of the terminal U.
The charging voltage and charging current of this repeated process over 6, which is caused by the AC power frequency between -4 and 4, are shown by the solid line ■l and the solid line in Figure 3! As shown in 1-4 to ■1-4, ■
. represents a predetermined voltage, and ts=tsti represents the time t! ~tl
;tl~tl,...+t@"-t@, each -j is equal time and corresponds to the conduction 01 cycle time of the control rectifying elements 2 and 3. The vertical axis (■) represents the charging current, and the pH discharge current The reason why the peak values of the current !, -1 to ■, and -4 in each charging cycle are different is that as charging progresses, the current of the transistor 18 decreases, and the amount of charge in the charging/discharging capacitor 7.8 changes in each cycle. This is because the conduction angle θ gradually increases and becomes smaller.
以上のようにして充放電コンデンサ7.8の充電が所定
の充電電圧vcに達すると、前記抵抗9.10の参続点
より前記直流電源15によって設定された基準電圧に相
当する電圧が前記比較増幅回路14の負側端に入力され
る。そしてこの比較増幅回路14の出力Fioあるいは
負とガシ前記トランジスタ18をオフ状態にする。When the charging and discharging capacitor 7.8 reaches the predetermined charging voltage vc as described above, a voltage corresponding to the reference voltage set by the DC power supply 15 is applied from the connection point of the resistor 9.10 to the comparison It is input to the negative end of the amplifier circuit 14. Then, the output Fio of the comparison amplifier circuit 14 or the negative transistor 18 is turned off.
したがって前記移相トランス5の二次側回路は開かね、
前記)f −) ノ4ルス発生回路26fd制御整tl
LllE子z 、 sの順方向バイアスのタイミングで
F1’−)パルスを出力せず前記整流制御素子2.3社
点弧せず、前記充放電コンデンサ7゜Iへの充電は停止
される。そしてレーザー光を照射する時には前記クロッ
ク発振回路21によ)クロックが出力され前記開閉回路
28によって前記スイッチ81は閉じられ、前記トリガ
回路J0によりて起動用トリガが発せられ前記充放電コ
ンデンサ1.8の充電分を前記7ラツシ具ランプ11へ
放電させる。第3図の実* P sはその放電電流波形
を示しTsFi時間を示す。Therefore, the secondary circuit of the phase shift transformer 5 cannot be opened.
(above) f-) No. 4 pulse generation circuit 26fd control adjustment tl
At the timing of the forward bias of the LllE element z, s, the F1'-) pulse is not outputted, the rectification control elements 2 and 3 are not fired, and charging to the charge/discharge capacitor 7°I is stopped. When irradiating laser light, the clock oscillation circuit 21 outputs a clock, the switching circuit 28 closes the switch 81, the trigger circuit J0 issues a starting trigger, and the charging/discharging capacitor 1.8 The amount of charge is discharged to the seven lash lamps 11. The symbol *Ps in FIG. 3 indicates the discharge current waveform and indicates the TsFi time.
このフラッシェランプ11の放電によって゛パルス幅の
広いパルス光が生じ、このノ4ルス光によりて前記レー
ザー物質12は励起され照射時間ノ長イレーザー党を発
する。The discharge of the flash lamp 11 generates pulsed light with a wide pulse width, and the laser substance 12 is excited by this pulsed light to emit an eraser with a long irradiation time.
次に14ルス幅の狭いパルス波形を発生させる場合には
、前記スイッチS1およびSSは開かれる。したがって
前記充放電コンデンサ7および抵抗25は回路系から切
シ離される。この状態で前述の幅の広いパルス波形を発
生させる場1合と同様の作用が行なわれる。その結果ま
す比較増幅回路14の出力に正の信号が出力される。Next, when generating a narrow pulse waveform with a width of 14 pulses, the switches S1 and SS are opened. Therefore, the charging/discharging capacitor 7 and the resistor 25 are disconnected from the circuit system. In this state, the same effect as in case 1 is performed when the wide pulse waveform described above is generated. As a result, a positive signal is output to the output of the comparison amplifier circuit 14.
この信号は′トランジスタ18を完全にオン状態にさせ
る信号である。したがって移相トランス5の二次側回路
は閉じられ、・主に移相コンデンサ19の容量と抵抗2
4の時定数に基づいた信号が前記移相トランス5の二次
側中点と移相コンデンサ19の出力−側との間に生じる
。そして、この2点間の信号がf−)パルス発生回路2
6に入力される。そこでこのf−トノ4ルス発生回11
126は第2図に示す0!の導通角で制御整流素子2,
3を制御する。ここに、θ1〉01となるのは前記抵抗
24と25との並列接続の値に対する抵抗24の単独の
値によって、移相トランス5の二次側回路の時定数が変
えられるからで、つまり抵抗24の単独使用の方が時定
数が長くなり、ダート/′?ルス発生回路26への入力
信号の立ち上がシがf!!わ、このe−)パルス発生回
路26からの前記制御整流素子Z、Sを導通状態にさせ
るダートパルス信号の送出が遅れるからである。しかる
にこの1サイクルの作用において、前記電源トランス4
の一次側あるいは二次側にwJ2図のCの様な電圧波形
あるい[dO様な電流波形が得られる。これら電圧ある
いは電流は前記整流回路6によって全波整流され前記充
放電コンデンサ8に充電される。そして、次の充電サイ
クルではこの充電電圧が前記抵抗9.10の接続点より
前記比較増幅回路14o負側端ヘフイードバツクさね、
正側端の基準電圧と比較されその差に応じた正出力を前
記トランジスタ18へ入力する。これによりトランジス
タ18の流す電流は前回充電サイクルよシ減少する。つ
まシトランジスタ18の抵抗分が増す。したがりて前記
移相トランス5の二次側回路の時定数は長くなり、結果
として前記制御整流素子2,3の導通角0重を減少させ
る。This signal is a signal that completely turns on the transistor 18. Therefore, the secondary side circuit of the phase shift transformer 5 is closed, mainly consisting of the capacitance of the phase shift capacitor 19 and the resistance 2.
A signal based on a time constant of 4 is generated between the middle point of the secondary side of the phase shift transformer 5 and the output side of the phase shift capacitor 19. Then, the signal between these two points is f-) pulse generation circuit 2
6 is input. Therefore, this f-tono 4 rus occurrence number 11
126 is 0! shown in FIG. The rectifying element 2 is controlled at a conduction angle of
Control 3. Here, θ1>01 because the time constant of the secondary side circuit of the phase shift transformer 5 can be changed by the independent value of the resistor 24 with respect to the value of the parallel connection of the resistors 24 and 25. If 24 is used alone, the time constant will be longer, and Dart/'? The rising edge of the input signal to the pulse generating circuit 26 is f! ! This is because e-) the transmission of the dart pulse signal from the pulse generating circuit 26 that brings the control rectifying elements Z and S into conduction is delayed. However, in this one cycle of action, the power transformer 4
A voltage waveform like C in the wJ2 diagram or a current waveform like [dO] can be obtained on the primary or secondary side of the circuit. These voltages or currents are full-wave rectified by the rectifier circuit 6 and charged to the charge/discharge capacitor 8. Then, in the next charging cycle, this charging voltage is fed back from the connection point of the resistor 9.10 to the negative side terminal of the comparison amplifier circuit 14o.
It is compared with the reference voltage at the positive side end, and a positive output corresponding to the difference is inputted to the transistor 18. This causes the current flowing through transistor 18 to decrease compared to the previous charging cycle. The resistance of the shoe transistor 18 increases. Therefore, the time constant of the secondary circuit of the phase shift transformer 5 becomes longer, and as a result, the conduction angle of the controlled rectifying elements 2 and 3 is reduced.
以上の充電サイクルのくり返しによって前記充放電コン
デンサ7への充電が行なわれる。そのにして前記充放電
コンデンサ8の充電が所定の充電電圧vcに達すると前
述の広いパルスを得る時と同様に充電が停止される。そ
、して前述のレーデ−光照射と同様の作用により短いパ
ルス幅をもつたレーザー光が発生する。なおこの時前記
フラッジ−ランプ11へ放電される電流波形を第3図の
点線P傘に示す。By repeating the above charging cycle, the charging/discharging capacitor 7 is charged. Then, when the charging of the charging/discharging capacitor 8 reaches a predetermined charging voltage vc, charging is stopped in the same way as when obtaining the wide pulse described above. Then, a laser beam with a short pulse width is generated by the same effect as the laser beam irradiation described above. The waveform of the current discharged to the flood lamp 11 at this time is shown by the dotted line P in FIG.
以上の様に各充を電圧を各サイクルで逐次フィードバッ
クし各サイクルでの充電の位相を変え、充電電流を制御
することによル、充放電コンデンサの容量が変化しても
所定の時間で正確な充電が行なわれるのである。なお、
上記実施例では充電サイクルを交流電源周波数に基づき
決めたが、別途に状況に応じた充電サイクルを設定して
も良い。As described above, by sequentially feeding back the charging voltage in each cycle, changing the charging phase in each cycle, and controlling the charging current, it is possible to maintain accuracy within a specified time even if the capacitance of the charging/discharging capacitor changes. Charging takes place. In addition,
In the above embodiment, the charging cycle is determined based on the AC power frequency, but a charging cycle may be set separately depending on the situation.
また、本発明は上記した実施例に限定されることはなく
その要旨を逸脱しない限り電源を単相、3相、多相いず
れの電源でも良く、また種?
参のパルス出力を必要とする装置にても応用出来るのは
もちろんである。Further, the present invention is not limited to the above-described embodiments, and the power source may be a single-phase, three-phase, or polyphase power source as long as it does not deviate from the gist of the invention. Of course, the present invention can also be applied to devices that require pulse output.
本発明によれば電源部と充放電部で構成されるノクルス
田力発生装置において、所望の・臂ルス出力を得るため
に行なう充放電容量の変化に対し、その充電サイクルを
均一化し各サイクルの充電量を制御することによってい
かなる容量にも対処出来る。すなわち容量が小さい時で
の短時間に所定電圧以上まで過充電を行なってしまうこ
とや容量が大きい時の長時間充電および充電回路の過大
電流などを考慮する必要がなく、t7’jDc−DCコ
ンバータの様な特別の電源を使用せず通常の商用電源に
て容量変化に関係なく充電電圧の精度が保てる。したが
りて柚々の/4ルス出力を要求される装置などにおいて
は最適なパルス出力を得ることが出来、その・母ルス出
力も質の良好なものが容易に得られるのである。%にレ
ーザー光による加工(例えば溶接など)においては、最
適なレーデ−光の提供を可能にし、その加工精度を上げ
ることか容易に夾現出来る。すなわち種々のパルスに要
求される精度を充分に満足させる装置を容易に実現可能
にする充放亀用電源装置を提供し得るものである。According to the present invention, in a Noculus field power generation device composed of a power source section and a charging/discharging section, the charging cycle is made uniform in response to changes in charging/discharging capacity that are performed to obtain a desired output. Any capacity can be handled by controlling the amount. In other words, there is no need to consider overcharging to a predetermined voltage or higher in a short period of time when the capacity is small, or long-term charging and excessive current in the charging circuit when the capacity is large. Charging voltage accuracy can be maintained regardless of capacitance changes using a normal commercial power source without using a special power source. Therefore, it is possible to obtain an optimal pulse output in a device that requires a /4 las output, and a good quality lasing output can be easily obtained. %, in processing (for example, welding) using laser light, it is possible to provide the optimum laser light, and it is easily possible to improve the processing accuracy. In other words, it is possible to provide a charging/discharging power supply device that can easily realize a device that fully satisfies the accuracy required for various pulses.
第1図は本発明に係わる実施例のTh成図、第2図は第
1図における1サイクルでの充電電流波形、充電電圧波
形および制御整流素子の導通角を示す図、第3図は第1
図における所定電圧までの充電−流、充%Lt圧の充電
過程の波形と放電の電流波形をそれぞれ示す図である。
2.3・・・制御整流素子、5・・・移相トランス、7
.8・・・充放電コンデンサ、19・・・移相コンデン
サ、26・・・グートノ臂ルス発生回路。
1人代理人 弁理士 鈴 江 武 彦
第1図FIG. 1 is a Th diagram of an embodiment of the present invention, FIG. 2 is a diagram showing the charging current waveform, charging voltage waveform, and conduction angle of the control rectifier in one cycle in FIG. 1, and FIG. 1
It is a figure which shows the waveform of the charge process of charge-current to the predetermined voltage, charge %Lt pressure, and the current waveform of discharge in a figure, respectively. 2.3... Control rectifying element, 5... Phase shift transformer, 7
.. 8... Charge/discharge capacitor, 19... Phase shift capacitor, 26... Good pulse generation circuit. Single agent Patent attorney Takehiko Suzue Figure 1
Claims (1)
れた充電サイクルの1サイクル内における制御された通
電位相で交流電源信号を通電し出力する制御整流部と、
この制御整流部の通電出力を基に充電が行なわれる使用
段数可変手段をもった複数の充放電部と、これら充放電
部の充電電圧を各充電サイクルにて逐次所定の基準電圧
と比較しその差に応じた信号を出力する比較部と、この
比較部の信号に応じて前記制御整流部の通電位相を制御
する位相制御部と、前記充放電部の使用段数可変手段に
応動し前記位相制御部の初期位相制御出力を決定する手
段と、この手段によって決定された初期通電位相で前記
充放電部の充電を開始し、前記位相制御部の各充電サイ
クルの位相制御出力に応じて充電を行ない所定の充電電
圧に達すると、充電を停止し放電体へ放電を行なうこと
を特徴とした充放電用電源装置。a means for determining a Marugame cycle; a control rectifier that energizes and outputs an AC power signal in a controlled energization phase within one charging cycle determined by the means;
A plurality of charging/discharging sections each having a means for varying the number of stages used perform charging based on the energization output of the control rectifying section, and the charging voltages of these charging/discharging sections are sequentially compared with a predetermined reference voltage in each charging cycle. a comparison section that outputs a signal according to the difference; a phase control section that controls the energization phase of the control rectification section according to the signal of the comparison section; means for determining an initial phase control output of the charging/discharging section, and charging of the charge/discharge section is started at the initial energization phase determined by the means, and charging is performed according to the phase control output of each charging cycle of the phase control section. A charging/discharging power supply device characterized by stopping charging and discharging to a discharge body when a predetermined charging voltage is reached.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56168974A JPS5872345A (en) | 1981-10-22 | 1981-10-22 | Charing and discharging power source |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56168974A JPS5872345A (en) | 1981-10-22 | 1981-10-22 | Charing and discharging power source |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5872345A true JPS5872345A (en) | 1983-04-30 |
| JPH035675B2 JPH035675B2 (en) | 1991-01-28 |
Family
ID=15878012
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56168974A Granted JPS5872345A (en) | 1981-10-22 | 1981-10-22 | Charing and discharging power source |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5872345A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR102008403B1 (en) * | 2018-12-28 | 2019-08-07 | 조용성 | Safe driving support system using traffic information detector installed on median strip and guard rail |
| KR102029070B1 (en) * | 2018-12-28 | 2019-10-07 | 조용성 | Safety driving support system that collects and provides traffic information affecting road driving through pilot lamp installed on median strip and guard rail |
-
1981
- 1981-10-22 JP JP56168974A patent/JPS5872345A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPH035675B2 (en) | 1991-01-28 |
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