JPH035675B2 - - Google Patents
Info
- Publication number
- JPH035675B2 JPH035675B2 JP56168974A JP16897481A JPH035675B2 JP H035675 B2 JPH035675 B2 JP H035675B2 JP 56168974 A JP56168974 A JP 56168974A JP 16897481 A JP16897481 A JP 16897481A JP H035675 B2 JPH035675 B2 JP H035675B2
- Authority
- JP
- Japan
- Prior art keywords
- charging
- discharging
- cycle
- section
- phase
- 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 - Lifetime
Links
- 238000007599 discharging Methods 0.000 claims description 38
- 239000003990 capacitor Substances 0.000 description 32
- 230000010363 phase shift Effects 0.000 description 17
- 230000007423 decrease Effects 0.000 description 6
- 238000010586 diagram Methods 0.000 description 4
- 239000000463 material Substances 0.000 description 4
- 230000010355 oscillation Effects 0.000 description 4
- 230000003111 delayed effect Effects 0.000 description 3
- 238000005516 engineering process Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 230000003287 optical effect Effects 0.000 description 2
- 230000001443 photoexcitation Effects 0.000 description 2
- 238000003466 welding Methods 0.000 description 2
- 238000005520 cutting process Methods 0.000 description 1
- 230000005284 excitation Effects 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 230000007774 longterm Effects 0.000 description 1
- 230000002265 prevention Effects 0.000 description 1
- 238000007493 shaping process Methods 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
Landscapes
- Lasers (AREA)
- Direct Current Feeding And Distribution (AREA)
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つ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) 従来の技術
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、放電によつてパルスを得
るようにしている。特にこの種の装置は、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、溝切り等の加工分野ではその用途も
広い。したがつて各加工用途に応じた照射エネ
ルギーや照射時間をもつたレーザー光が必要と
なり、その手段として従来、前記の充放電コン
デンサの充電電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電は停止される様にな
つている。(2) Conventional technology In general, devices for easily obtaining pulses include:
It consists of a power supply section and a charging/discharging capacitor, and pulses are obtained by charging and discharging the charging/discharging capacitor. In particular, this type of device 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. Therefore, a laser beam with irradiation energy and irradiation time suitable for each processing application is required, and as a means of achieving this, conventionally, the charging voltage and number of stages used in the charging/discharging capacitor described above are changed, and the laser beam is adjusted according to each application. 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. ,
All that is needed is to shorten the photoexcitation time. In this case, when the charging/discharging capacitor is discharging, charging to the charging/discharging capacitor from the power supply section 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
御回路を用いて充電電流と充電電圧をフイード
バツ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
コンバータによつて直流充電を行なつたりする
ものがある。 Also, when charging, if a 50/60Hz commercial frequency is used as a charging power source, there are some that use an AC phase control circuit to feed back the charging current and charging voltage, and others that convert the commercial power source to DC. , this is a high frequency DC-DC
Some converters can perform DC charging.
(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りの充電時間
が大幅に変化し、これに対応を取らせるための充
電制御は非常に困難であつた。したがつて充電の
精度が悪くなり、よつて放電の安定度も悪くなつ
て所望のレーザー光を得られない欠点を根本的に
もつている。(3) Problems with the conventional technology In the conventional technology described above, when the number of stages of charging/discharging capacitors used changes significantly, the charging time from the power supply section changes significantly, and charging control to deal with this changes significantly. It was extremely difficult. Therefore, the accuracy of charging deteriorates, and the stability of discharging also deteriorates, 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、フイードバツクの時間遅れに
よ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電流および過充
電はまぬがれなく、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
いては回路が複雑となり製作上好ましくない。 In addition, although the above-mentioned fundamental drawbacks are taken into consideration, overcurrent and overcharging are inevitable when the discharge capacitor has a large capacity or a small capacity due to the instability of the control circuit due to the feedback time delay. , it is difficult to improve charging accuracy. Furthermore, when using a DC-DC converter, the circuit becomes complicated, which is not desirable in terms of manufacturing.
(4) 発明の目的
本発明は充放電部の容量変化に対しても均一な
高い精度で充電が行なえよつて安定な放電状態を
得られる製作上簡単な充放電用電源装置を提供す
ることにある。(4) Purpose of the Invention The object of the present invention is to provide a charging/discharging power supply device that is easy to manufacture and can perform charging uniformly and with high precision even when the capacitance of the charging/discharging section changes, thereby obtaining a stable discharging state. be.
(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部にて基準電
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電位相を制御して所定の充
電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り上記
目的を達成するものである。(5) Key Points of the Invention The present invention, when charging the charging/discharging section, performs charging in a predetermined charging cycle, sequentially detects the charging voltage in each charging cycle, compares it with a reference voltage in a comparison amplifier section, and calculates the charging voltage. The phase of energization to the charging/discharging unit in each charging cycle is controlled in accordance with the comparison signal to charge to a predetermined charging voltage. Further, 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) 発明の実施例
次に本発明の一実施例を第1図、第2図および
第3図を用いて説明する。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。端子U
と端子Vおよび端子Uと端子Wは交流電源端子
で、端子U〜W間にはラツシユ電流防止用コイル
1と、極性を逆にして並列接続した制御整流素子
2,3(サイリスタなど)と、電源トランス4の
一次側とが直列に接続されている。また前記端子
U〜V間には移相トランス5の一次側が接続され
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。そして前記電源トラン
ス4の二次側には整流回路6が接続され、この整
流回路6の出力両端には充放電用コンデンサ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サ7はスイツ
チS1を介して整流回路6と接続される様になつて
いる。さらに前記放電管11の近傍には同放電管
11からのパ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の光を反射する一方が
半鏡面、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。また14は所定の基準電圧と充電電
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、正側端には直流電源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ツチS2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の信号に応じて電流制御をするトラ
ンジスタ18のベース側が接続されている。(6) Embodiment of the Invention Next, an embodiment of the present invention will be described with reference to FIGS. 1, 2, and 3. Note that FIG. 1 shows a configuration diagram, and FIGS. 2 and 3 show characteristic diagrams. Terminal U
and terminal V, and terminals U and W are AC power supply terminals, and between terminals U and W there is a lash current prevention coil 1, and control rectifying elements 2 and 3 (such as a thyristor) connected in parallel with reversed polarity. The primary side of the power transformer 4 is connected in series. Further, the primary side of a phase shift transformer 5 is connected between the terminals U to V. The charging cycle is determined based on the AC frequency between the terminals U to V. A rectifier circuit 6 is connected to the secondary side of the power transformer 4, and a charging/discharging capacitor 7,
8, a series circuit of resistors 9 and 10, and a discharge tube 11 for emitting discharge light are connected in parallel with each other. The charging/discharging capacitor 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 pulsed light from the discharge tube 11 is installed, and one half of the laser material 12 reflects the light on the optical axis of the laser material 12. A pair of resonant mirrors 13, one with a mirror surface and the other with a mirror surface, are installed so as to face each other with the laser material 12 interposed therebetween. Reference numeral 14 denotes a comparison amplifier circuit that compares a predetermined reference voltage with a charging voltage.The common connection portion of the resistors 9 and 10 is connected to the negative side input terminal of this comparison amplifier circuit 14, and to the positive side terminal. A sliding portion of a reference voltage adjusting resistor 17 applied from a DC power supply 15 via a resistor 16 is connected. Further, an adjusting resistor 17 is connected to both ends of this reference voltage adjusting resistor 17.
A switch S 2 is connected which short-circuits the applied voltage of. The output side of the comparison amplifier circuit 14 is connected to the base side of a transistor 18 that controls current according to the signal of the comparison amplifier circuit 14.
一方、前記移相トランス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20,21,22,23によつて形成された
ブリツジ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, and diodes 20, 21, 22, 23 are connected between this output side and the other end of the secondary side of the phase shifting transformer 5. The input terminal of a bridge rectifier circuit formed by is connected.
さらにこのブリツジ整流回路の出力側の一端は
抵抗24を介して前記トランジスタ18のコレク
タ側に接続され、もう一端はエミツタ側に接続さ
れている。なお、前記抵抗24には抵抗25がス
イツチS3を介して並列に接続される様になつてお
り、またスイツチS3と前記スイツチS1とは連動さ
れている。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
圧差によつてゲートパルスを出力するゲートパル
ス発生回路26が移相トランス5の2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
力によつて前記制御整流素子2,3は動作を行な
う様になつている。 Furthermore, one end of the output side of this bridge rectifier circuit is connected to the collector side of the transistor 18 via a resistor 24, and the other end is connected to the emitter side. Note that a resistor 25 is connected in parallel to the resistor 24 via a switch S3 , and the switch S3 and the switch S1 are interlocked. Further, a gate pulse generation circuit 26 that outputs a gate pulse based on 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 secondary side of the phase shifting transformer 5. It is connected to the middle point of the side and the output side of the phase shifting capacitor 19. The control rectifying elements 2 and 3 are operated by the output of the gate pulse generating circuit 26.
また、27はフラツシユランプ11の放電開始
用のクロツク発振回路で、このクロツク発振回路
27には前記スイツチS2の開閉を行なう開閉回路
28が接続され、この開閉回路28にはフラツシ
ユランプ11に外巻されたトリガ電極29を介し
てフラツシユランプ11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。 Reference numeral 27 denotes a clock oscillation circuit for starting discharge of the flash lamp 11. A switching circuit 28 for opening and closing the switch S2 is connected to this clock oscillation circuit 27. A trigger circuit 30 for providing a starting trigger to the flash lamp 11 is connected via a trigger electrode 29 wound externally to the flash lamp 11 .
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パルス波形を発生させる
場合には、前記スイツチS1およびS2は閉じられて
いる。この状態で充電を行なう場合、前記クロツ
ク発振回路27からクロツク信号は出力されず、
したがつてスイツチS2は開状態にある。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によつて設定された基準電圧が入力される。
したが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5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
号が前記ゲートパルス発生回路26に入力され
る。そしてこのゲートパルス発生回路26は第2
図に示すθ1の導通角で前記制御整流素子2,3を
制御する。以上により1サイクルにおいて、前記
電源トランス4の一次側あるいは二次側には第2
図のa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
るいは電流は前記移相トランス4の二次側の整流
回路6によつ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。以上により充電された電
圧は前記抵抗9,10の接続点より前記比較増幅
回路14の負側端にフイードバツクされ、前記と
同様に正側端の基準電圧と比較される。この時負
側端電圧と正側端電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1
4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。したがつて前記移相トラン
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つて生じた抵抗
分で決定され、前記ゲートパルス発生回路26へ
の入力は遅れる。したがつて前記制御整流素子
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7,8への充電量は減少する。以上の
ような作用のくり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〜V間の交流電源周波数に起因するもので
ある。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V1および実線I1-1〜I1-4に
示す。なお、Vcは所定電圧を、t1〜t6は時刻を示
しt1〜t2、t2〜t3、…、t5〜t6の各間は等時間で前
記制御整流素子2,3の導通の1サイクル時間に
相当する。また縦軸Iは充電電流を、Pは放電電
流を示し、各充電サイクルでの電流I1-1〜I1-4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θ1が小さくなるからである。 Next, the apparatus configured as above will be explained. First, when generating a pulse waveform with a wide pulse width, the switches S1 and S2 are closed. When charging is performed in this state, no clock signal is output from the clock oscillation circuit 27,
Switch S2 is therefore in the open state. And when alternating current is applied between terminal UV and terminal UW,
A reference voltage set by the DC power supply 15 is input to the positive side end of the comparison amplifier circuit 14 .
Therefore, a positive signal is outputted from the comparison amplifier circuit 14, and the transistor 18 is completely turned on. That is, a closed circuit is formed in the secondary side circuit of the phase shift transformer 5 through the transistor 18, and a signal based mainly on the time constant of the capacitance of the phase shift capacitor 19 and the parallel resistance of the resistors 24 and 25 is generated. This occurs between the middle point of the secondary side of the phase shift transformer 5 and the output side of the phase shift capacitor 19. A signal between these two points is input to the gate pulse generation circuit 26. This gate pulse generation circuit 26 is connected to the second
The control rectifying elements 2 and 3 are controlled at a conduction angle of θ 1 shown in the figure. As described above, in one cycle, the primary side or the secondary side of the power transformer 4 is connected to the secondary side.
A voltage waveform like a in the figure or a current shaping like b in the figure can be obtained. Note that the sine wave UW is a power waveform between terminals U and W. The voltage or current thus obtained is full-wave rectified by the rectifier circuit 6 on the secondary side of the phase shift transformer 4, and charged into the charging/discharging capacitors 7, 8. The voltage charged in the above manner 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 voltage and the positive end voltage is smaller than that during the charging cycle. Therefore, comparison amplifier circuit 1
The output of 4 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 determined by the phase shift capacitor 9, the parallel resistance of the resistors 24 and 25, and the resistance caused by the decrease in the collector current of the transistor 18. , the input to the gate pulse generation circuit 26 is delayed. The conduction angle of the controlled rectifying elements 2, 3 therefore decreases. In other words, the amount of charge to the charge/discharge capacitors 7, 8 decreases. Charging to a predetermined voltage is performed by repeating the above-described actions. Note that this repetition period is caused by the AC power frequency between the terminals U to V. The charging voltage and charging current of this repeated process are shown by the solid line V 1 and the solid lines I 1-1 to I 1-4 in FIG. 3. Incidentally , Vc represents a predetermined voltage , and t1 to t6 represent time, and the control rectifying element 2 , This corresponds to one cycle time of conduction of 3. Further, the vertical axis I indicates the charging current, and P indicates the discharging current. The reason why the peak values of the currents I 1-1 to I 1-4 in each charging cycle are different is because the current of the transistor 18 decreases as charging progresses. This is because the amount of charge in the charging and discharging capacitors 7 and 8 increases successively in each cycle, and the conduction angle θ 1 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の接続点より前記直流電源15によつて設定
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の出力は0あるいは負となり前記トラ
ンジスタ18をオフ状態にする。したがつて前記
移相トランス5の二次側回路は開かれ、前記ゲー
トパルス発生回路26は制御整流素子2,3の順
方向バイアスのタイミングではゲートパルスを出
力せず前記整流制御素子2,3は点弧せず、前記
充放電コンデンサ7,8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ツク
発振回路27によりクロツクが出力され前記開閉
回路28によつて前記スイツチS2は閉じられ、前
記トリガ回路30によつて起動用トリガが発せら
れ前記充放電コンデンサ7,8の充電分を前記フ
ラツシユランプ11へ放電させる。第3図の実線
P1はその放電電流波形を示しT1は時間を示す。
このフラツシユランプ11の放電によつてパルス
幅の広いパルス光が生じ、このパルス光によつて
前記レーザー物質12は励起され照射時間の長い
レーザー光を発する。 When the charging and discharging capacitors 7 and 8 reach the predetermined charging voltage V c as described above, the resistors 9 and
A voltage corresponding to the reference voltage set by the DC power supply 15 is inputted to the negative end of the comparison amplifier circuit 14 from the connection point 10 . The output of the comparison amplifier circuit 14 becomes 0 or negative, turning off the transistor 18. Therefore, the secondary side circuit of the phase shift transformer 5 is opened, and the gate pulse generating circuit 26 does not output a gate pulse at the forward bias timing of the control rectifiers 2, 3, does not ignite, and charging to the charging/discharging capacitors 7 and 8 is stopped.
When irradiating the laser beam, the clock oscillation circuit 27 outputs a clock, the switching circuit 28 closes the switch S2 , the trigger circuit 30 issues a starting trigger, and the charging/discharging capacitor 7 , 8 is discharged to the flash lamp 11. Solid line in Figure 3
P 1 indicates the discharge current waveform, and T 1 indicates the time.
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 laser light with a long irradiation time.
次にパルス幅の狭いパルス波形を発生させる場
合には、前記スイツチS1およびS3は開かれる。し
たがつて前記充放電コンデンサ7および抵抗25
は回路系から切り離される。この状態で前述の幅
の広いパルス波形を発生させる場合と同様の作用
が行なわれる。その結果まず比較増幅回路14の
出力に正の信号が出力される。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。したがつて移相トランス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点間の信号がゲート
パルス発生回路26に入力される。そこでこのゲ
ートパルス発生回路26は第2図に示すθ2の導通
角で制御整流素子2,3を制御する。ここに、θ1
>θ2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の単独の値によつて、、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、ゲートパルス発生回路26への入力
信号の立ち上がりが遅れ、このゲートパルス発生
回路26からの前記制御整流素子2,3を導通状
態にさせるゲ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
に第2図のcの様な電圧波形あるいはdの様な電
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によつ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14の負側端へフイード
バツクされ、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
回充電サイクルより減少する。つまりトランジス
タ18の抵抗分が増す。したがつて前記移相トラ
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θ2を減少さ
せる。以上の充電サイクルのくり返しによつて前
記充放電コンデンサ7への充電が行なわれる。そ
の充電電圧波形および充電電流を第3図の点線
V2および点線I2-1〜I2-4に示す。以上の様にして
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。そして前述のレーザー光照
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ツシユラ
ンプ11へ放電される電流波形を第3図の点線
P2に示す。 Next, when generating a pulse waveform with a narrow pulse width, the switches S1 and S3 are opened. Therefore, the charging/discharging capacitor 7 and the resistor 25
is separated from the circuit system. In this state, the same effect as in the case of generating the wide pulse waveform described above is performed. As a result, first, a positive signal is output to the output of the comparison amplifier circuit 14. This signal is a signal that turns transistor 18 completely on. Therefore, the secondary side circuit of the phase shift transformer 5 is closed and mainly consists of the capacitance of the phase shift capacitor 19 and the resistor 2.
A signal based on the time constant of 4 is transmitted to the phase shift transformer 5.
occurs between the midpoint of the secondary side of and the output side of the phase shift capacitor 19. The signal between these two points is then input to the gate pulse generation circuit 26. Therefore, this gate pulse generating circuit 26 controls the control rectifying elements 2 and 3 at a conduction angle of θ 2 shown in FIG. Here, θ 1
>θ 2 because the time constant of the secondary circuit of the phase shift transformer 5 can be changed depending on the value of the resistor 24 alone with respect to the value of the parallel connection of the resistors 24 and 25. When 24 is used alone, the time constant is longer, the rise of the input signal to the gate pulse generation circuit 26 is delayed, and the gate pulse signal from the gate pulse generation circuit 26 makes the control rectifiers 2 and 3 conductive. This is because the sending of the data is delayed. However, in this one cycle action, a voltage waveform as shown in c or a current waveform as shown in d in FIG. 2 is obtained on the primary or secondary side of the power transformer 4. 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 resistors 9 and 10 to the negative end of the comparison amplifier circuit 14, and compared with the reference voltage at the positive end, and a positive output is generated according to the difference. input to the transistor 18; As a result, the current flowing through transistor 18 is reduced compared to the previous charging cycle. In other words, the resistance of 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 θ 2 of the controlled rectifying elements 2 and 3 is reduced. By repeating the above charging cycle, the charging/discharging capacitor 7 is charged. The charging voltage waveform and charging current are shown by the dotted lines in Figure 3.
V 2 and dotted lines I 2-1 to I 2-4 . As described above, the charging and discharging capacitor 8 is charged to a predetermined charging voltage.
When V c is reached, charging is stopped in the same way as when obtaining the wide pulse described above. Laser light with a short pulse width is generated by the same action as the laser light irradiation described above. At this time, the current waveform discharged to the flash lamp 11 is shown by the dotted line in FIG.
Shown on P 2 .
以上の様に各充電電圧を各サイクルで逐次フイ
ードバツ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り、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, each charging voltage is sequentially fed back in each cycle, and the charging phase in each cycle is changed.
By controlling the charging current, accurate charging can be performed within a predetermined time even if the capacitance of the charging/discharging capacitor changes. 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、また種々のパ
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 unless it deviates from the gist, the present invention can be applied to a single-phase power supply,
It goes without saying that either a three-phase or multi-phase power source may be used, and it can also be applied to devices that require various pulse outputs.
(7) 発明の効果
本発明によれば電源部と充放電部で構成される
パルス出力発生装置において、所望のパルス出力
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
制御することによつ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つ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、またDC−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。したがつて種々のパ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、そのパルス出力も質の良好なものが容易に
得られるのである。特にレーザー光による加工
(例えば溶接など)においては、最適なレーザー
光の提供を可能にし、その加工精度を上げること
が容易に実現出来る。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
現可能にする充放電用電源装置を提供し得るもの
である。(7) Effects of the Invention According to the present invention, in a pulse output generation device composed of a power source section and a charging/discharging section, the charging cycle can be made uniform in response to changes in charging/discharging capacity that are performed to obtain a desired pulse output. Any capacity can be handled by controlling the amount of charge in each cycle. In other words, there is no need to consider overcharging to a specified voltage or higher in a short period of time when the capacity is small, or long-term charging or 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, in devices that require various pulse outputs, it is possible to obtain the optimum pulse output, and the pulse output can also be easily obtained with good quality. Particularly in processing using laser light (for example, welding, etc.), it is possible to provide the optimum laser light and easily 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構成図、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
充電電流、充電電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……ゲートパルス発生回路。
Fig. 1 is a configuration diagram of an embodiment related to the present invention;
The figure shows the charging current waveform, charging voltage waveform, and conduction angle of the control rectifier in one cycle in Figure 1, and Figure 3 shows the charging process waveform of the charging current and charging voltage up to a predetermined voltage in Figure 1. FIG. 3 is a diagram showing current waveforms of discharge and discharge, respectively. 2, 3... Control rectifier, 5... Phase shift transformer, 7, 8... Charge/discharge capacitor, 19... Phase shift capacitor, 26... Gate pulse generation circuit.
Claims (1)
つて決めら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
つ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、この手段によつて決
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。1 A means for determining a charging cycle, a control rectifier that energizes and outputs an AC power signal in a controlled energization phase within one cycle of the charge cycle determined by the means, and a energization output of the control rectifier. A plurality of charging/discharging sections each having a means for varying the number of stages used, and charging voltages of these charging/discharging sections are sequentially compared with a predetermined reference voltage in each charging cycle, and a signal corresponding to the difference is output. a comparison section, a phase control section that controls the energization phase of the control rectification section in response to a signal from the comparison section, and an initial phase control output of the phase control section that is determined in response to a means for varying the number of stages used in the charging/discharging section. and a means for starting charging of the charging/discharging section at an initial energization phase determined by the means, and charging according to a phase control output of each charging cycle of the phase control section to reach a predetermined charging voltage. Then, the charging/discharging power supply device stops charging and discharges to the discharge body.
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 JPS5872345A (en) | 1983-04-30 |
| JPH035675B2 true 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) |
Cited By (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
Cited By (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 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5872345A (en) | 1983-04-30 |
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