JPH0413951B2 - - Google Patents
Info
- Publication number
- JPH0413951B2 JPH0413951B2 JP57034274A JP3427482A JPH0413951B2 JP H0413951 B2 JPH0413951 B2 JP H0413951B2 JP 57034274 A JP57034274 A JP 57034274A JP 3427482 A JP3427482 A JP 3427482A JP H0413951 B2 JPH0413951 B2 JP H0413951B2
- Authority
- JP
- Japan
- Prior art keywords
- voltage
- terminal
- gap
- discharge
- main 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 - Lifetime
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Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03K—PULSE TECHNIQUE
- H03K3/00—Circuits for generating electric pulses; Monostable, bistable or multistable circuits
- H03K3/02—Generators characterised by the type of circuit or by the means used for producing pulses
- H03K3/53—Generators characterised by the type of circuit or by the means used for producing pulses by the use of an energy-accumulating element discharged through the load by a switching device controlled by an external signal and not incorporating positive feedback
- H03K3/537—Generators characterised by the type of circuit or by the means used for producing pulses by the use of an energy-accumulating element discharged through the load by a switching device controlled by an external signal and not incorporating positive feedback the switching device being a spark gap
Landscapes
- Generation Of Surge Voltage And Current (AREA)
Description
【発明の詳細な説明】
本発明は急峻波衝撃電圧発生装置(以下急峻波
発生装置という)に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a steep wave impulse voltage generator (hereinafter referred to as a steep wave generator).
急峻波衝撃電圧試験として高電圧の波頭長50ns
〜200ns、波尾長0.2μs〜1μsのような急峻な立上
りパルス電圧波形が要求される。このような急峻
波発生装置は極めて低インダクタンス化が要求さ
れるため、回路素子は構造も含めて小形化が必要
となる。また小形化とともに絶縁も高耐電圧絶縁
材料が必要となる。 High voltage wavefront length 50ns for steep wave impact voltage test
A steep rising pulse voltage waveform of ~200 ns and a wave tail length of 0.2 μs to 1 μs is required. Since such a steep wave generator is required to have extremely low inductance, the circuit elements, including their structure, must be miniaturized. In addition, with miniaturization, high voltage insulation materials are required for insulation.
球電極間隙の放電を利用した急峻波発生装置は
球間隙1〜2段のものがあるが、高電圧になれば
なるほど球電極の直径が大きくなり制作費が高価
になる。球間隙1〜2段のものを高電圧化してい
くと始動特性が極端に悪くなり、急峻波衝撃電圧
波形が得られないような回路定数になつてしまう
などの欠陥を内蔵している。 There are steep wave generators that utilize discharge between spherical electrodes and have one or two stages of spherical gaps, but the higher the voltage, the larger the diameter of the spherical electrodes and the higher the manufacturing cost. If the voltage is increased to one or two stages of ball gaps, the starting characteristics will become extremely poor, and the circuit constants will become such that a steep impulse voltage waveform cannot be obtained.
従来の球間隙1段の急峻波発生装置は、その回
路図を第1図に示すように構成されており、Cは
王コンデンサ、Aは高圧端子、Bは出力端子、R
は放電抵抗、Fは低圧結線バーである。Q1,Q2
は球電極で、Gは球電極Q1とQ2の球間隙で、こ
の間に放電を起こさせるようになつている。また
低圧側の帰還回路として低圧結線バーFによつて
放電抵抗Rの低圧端子Dと主コンデンサCの低圧
端子Iとを接続結線されている。 The circuit diagram of a conventional steep wave generator with one stage of sphere gap is constructed as shown in Figure 1, where C is a capacitor, A is a high voltage terminal, B is an output terminal, and R is a high voltage terminal.
is a discharge resistor, and F is a low voltage connection bar. Q1 , Q2
is a spherical electrode, and G is a spherical gap between spherical electrodes Q 1 and Q 2 , between which a discharge is caused. Further, as a feedback circuit on the low voltage side, a low voltage terminal D of the discharge resistor R and a low voltage terminal I of the main capacitor C are connected by a low voltage connection bar F.
この場合の動作説明を行うと、主コンデンサC
に充電端子TR1よりパルス電圧を充電する。それ
は高圧端子Aと出力端子Bの間にパルス電圧を印
加したことになる。主コンデンサCの充電電圧が
最高に達したところで、球電球Q1とQ2の球間隙
Gで自爆放電するような球間隙を保つておき放電
を起こさせる。高圧端子Aと出力端子Bの間が短
絡されたことになり、主コンデンサCの電位が急
峻波衝撃電圧波形の波尾を決める回路素子放電抵
抗Rの高圧部(出力端子B)に移行する。主放電
回路の低圧側は放電抵抗Rの低圧端子Dより低圧
結線バーFを通して主コンデンサCの低圧端子I
へ帰還する。出力端子Bは急峻波衝撃電圧試験を
行なう場合の被試験物接続端子である。この従来
の急峻波発生装置の欠陥は高電圧化する場合1段
で球間隙を長くとるため放電時間の遅れが生じ、
急峻波衝撃電圧波形の立上り部の波頭長が長くな
り、所定の急峻波衝撃電圧波形が得られなくな
る。そして放電のばらつきが著しく増加する。し
たがつて急峻波衝撃電圧が経済性および発生波形
の面において限定され、そして始動特性は幅のせ
まい特性となるなどの欠陥があつた。 To explain the operation in this case, the main capacitor C
Then, charge the pulse voltage from the charging terminal T R1 . This means that a pulse voltage is applied between the high voltage terminal A and the output terminal B. When the charging voltage of the main capacitor C reaches its maximum, a gap G between the bulbs Q 1 and Q 2 is maintained to cause a self-destructive discharge to occur. Since the high voltage terminal A and the output terminal B are short-circuited, the potential of the main capacitor C is transferred to the high voltage part (output terminal B) of the circuit element discharge resistor R that determines the tail of the steep impulse voltage waveform. The low voltage side of the main discharge circuit is connected to the low voltage terminal D of the discharge resistor R through the low voltage connection bar F to the low voltage terminal I of the main capacitor C.
Return to. Output terminal B is a test object connection terminal when performing a steep wave impact voltage test. The drawback of this conventional steep wave generator is that when increasing the voltage, the gap between the balls is made longer in one stage, which causes a delay in the discharge time.
The wavefront length of the rising portion of the steep impulse voltage waveform becomes longer, making it impossible to obtain a predetermined steep impulse voltage waveform. And the dispersion of discharge increases significantly. Therefore, the steep wave impulse voltage was limited in terms of economy and generated waveform, and the starting characteristics were short in width.
本発明はこれらの欠陥を排除して、幅のある著
しく改善した始動特性と、従来では出せなかつた
高電圧および安定した確実な急峻波衝撃電圧が得
られる急峻波発生装置を提供しようとするもので
ある。 The present invention aims to eliminate these deficiencies and provide a steep wave generator that can provide a wide range of significantly improved starting characteristics, a high voltage that could not be produced in the past, and a stable and reliable steep wave shock voltage. It is.
以下、本発明を第2図〜第3図に示す実施例に
より説明する。 The present invention will be explained below with reference to embodiments shown in FIGS. 2 and 3.
第2図は急峻波発生装置の回路図で、Cは主コ
ンデンサ、Aは高圧端子、Bは出力端子、Rは放
電抵抗、Fは低圧結線バー、Lはパルス伝送用コ
イル、Xは被試験物である。Q22は絶縁針端付半
球電極、Q1…Q(o+1)1は半球電極で、半球電極Q21
とQ22、Q31とQ32…Qo1とQo2はそれぞれ電気的に
接続され、中間接続電極W1…W(o-1)がその間か
ら導出されている。G1,G2…Goは半球電極Q1と
Q21、Q22とQ31…Qo2とQ(o+1)1のそれぞれの球間隙
で、この間に放電を起こさせるようになつてい
る。また球間隙G1のギヤツプ長は常に他の球間
隙G2…Goのギヤツプ長の2分の1に設定されて
いる。 Figure 2 is a circuit diagram of the steep wave generator, where C is the main capacitor, A is the high voltage terminal, B is the output terminal, R is the discharge resistor, F is the low voltage connection bar, L is the pulse transmission coil, and X is the test object. It is a thing. Q 22 is a hemispherical electrode with an insulated needle end, Q 1 …Q (o+1)1 is a hemispherical electrode, and hemispherical electrode Q 21
and Q 22 , Q 31 and Q 32 . . . Q o1 and Q o2 are electrically connected, respectively, and intermediate connection electrodes W 1 … W (o-1) are led out between them. G 1 , G 2 ...G o is hemispherical electrode Q 1 and
Q 21 , Q 22 and Q 31 ...A discharge is caused between the spheres of Q o2 and Q (o+1)1 , respectively. Further, the gap length of the spherical gap G 1 is always set to one half of the gap length of the other spherical gaps G 2 . . . G o .
C11…C1(o-2)は高圧端子Aと出力端子Bの接続
回路に一つおきに中間電極W1…W(o-2)を接続し、
その各接続点の前後に挿入された分圧用コンデン
サC21…C2(o-2)は高圧端子Aと出力端子Bの間に
残つている中間接続電極W2…W(o-3)、W(o-1)とを
接続する。 C 11 ...C 1 (o-2) connects every other intermediate electrode W 1 ...W (o-2) to the connection circuit between high voltage terminal A and output terminal B,
The voltage dividing capacitors C 21 ...C 2 (o-2) inserted before and after each connection point connect the intermediate connection electrodes W 2 ...W (o-3) remaining between the high voltage terminal A and the output terminal B, Connect with W (o-1) .
本装置の1設計例を示すと、半球電極Q1…
Q(o+1)1の直径を15cmとすると、コンデンサの静電
容量はC11とC2(o-2)は1000pF、C12…C1(o-2)、C21
…C2(o-3)は500pFとし、コンデンサC12…G2(o-3)の
印加電圧をコンデンサC11とC2(o-2)の印加電圧の
2倍になるようにする。このコンデンサの静電容
量はこの値に固定されるものでなく、半球電極の
直径などにより適宜選べばよい。 One design example of this device is a hemispherical electrode Q 1 ...
If the diameter of Q (o+1)1 is 15 cm, the capacitance of the capacitor is C 11 and C 2(o-2) is 1000 pF, C 12 …C 1(o-2) , C 21
...C 2 (o-3) is 500 pF, and the voltage applied to the capacitor C 12 ...G 2 (o-3) is set to be twice the voltage applied to the capacitors C 11 and C 2 (o-2) . The capacitance of this capacitor is not fixed to this value, but may be appropriately selected depending on the diameter of the hemispherical electrode, etc.
このような条件で主コンデンサCに充電端子
TR1より高電圧のパルスを充電する。それは高圧
端子Aと出力端子Bの間に高電圧のパルスを印加
したことになり、コンデンサC11…C1(o-2)、C21…
C2(o-2)によつて分圧され、各球間隙G1…Goには
等電圧が印加される。 Under these conditions, the charging terminal is connected to the main capacitor C.
Charge the pulse with a higher voltage than T R1 . This means that a high voltage pulse is applied between high voltage terminal A and output terminal B, and capacitors C 11 ...C 1(o-2) , C 21 ...
The voltage is divided by C 2(o-2) , and an equal voltage is applied to each spherical gap G 1 ...G o .
主コンデンCの電位が高圧パルス電圧の最高に
達したところでトリガーパルス端子TR2にトリガ
ーパルス電圧を印加し、パルス伝送用コイルLを
通して球間隙G2に放電を起こさせると、半球電
極Q22、Q1の電位が半球電極Q31の電位と同じに
なり、球間隔G1のギヤツプ長を他の球間隙のギ
ヤツプ長の2分の1に設定されているので、球間
隙G1には他の球間隙の印加電圧の2倍の電位傾
度の電圧が印加されることになり、球間隙G1に
自動的に放電が起こる。 When the potential of the main capacitor C reaches the highest high-voltage pulse voltage, a trigger pulse voltage is applied to the trigger pulse terminal T R2 to cause a discharge in the spherical gap G 2 through the pulse transmission coil L, and the hemispherical electrode Q 22 , Since the potential of Q 1 is the same as the potential of hemispherical electrode Q 31 and the gap length of the sphere gap G 1 is set to half of the gap length of the other sphere gaps, there is no other gap in the sphere gap G 1 . A voltage with a potential gradient twice that of the voltage applied to the sphere gap G 1 is applied, and a discharge automatically occurs in the sphere gap G 1 .
これにより球間隙G3にも最初の印加電圧の2
倍が印加されることになり、球間隙G3も自動的
に放電が起こる。このようにして高圧端子Aと出
力端子Bの間が短絡される。この場合の放電は従
来例の場合と異なり、トリガパルス端子TR2より
トリガーパルス電圧を印加し、トリガー電極の絶
縁針端付半球電極Q22と半球電極Q31の間の球間
隙G2に放電させることにより、次段球間隙の間
隙電圧を2倍以上に上昇させ、放電時間の遅れ、
放電のバラツキを少なくして安定した放電を起こ
させることができる。また任意に制御した遅延時
間のトリガーパルスをトリガーパルス端子TR2に
入れて安定放電が得られ、始動特性の著しい向上
が計れる。このような直列多段球間隙で高圧端子
Aと出力端子Bの間が短絡されたことになり、急
峻波衝撃電圧波形の波尾を決める放電抵抗Rの高
圧部(出力端子B)に主コンデンサCの電位が移
行する。そして主放電回路の低圧側は、放電抵抗
の低圧端子Dより低圧結線バーFを通して主コン
デンサの低圧端子Iへ帰還する。出力端子Bは急
峻波衝撃電圧試験を行なう場合の試験物接続端子
である。パルス伝送用コイルLは直列多段球間隙
G1…Goが放電動作時、主コンデンサCの電位が
移行するが、急峻波に対して高インピーダンス化
して高耐電圧を計つている。 As a result, the ball gap G 3 also becomes 2 of the initial applied voltage.
As a result, a discharge will automatically occur in the sphere gap G3 . In this way, high voltage terminal A and output terminal B are short-circuited. The discharge in this case is different from that of the conventional example. A trigger pulse voltage is applied from the trigger pulse terminal T R2 , and a discharge occurs in the spherical gap G 2 between the hemispherical electrode Q 22 with an insulated needle end of the trigger electrode and the hemispherical electrode Q 31 . By increasing the gap voltage of the next stage bulb gap more than twice, the discharge time is delayed,
It is possible to reduce variations in discharge and cause stable discharge. In addition, by inputting a trigger pulse with an arbitrarily controlled delay time to the trigger pulse terminal T R2 , stable discharge can be obtained, and the starting characteristics can be significantly improved. This means that the high voltage terminal A and the output terminal B are short-circuited due to the gap between the series multi-stage balls, and the main capacitor C is connected to the high voltage part (output terminal B) of the discharge resistor R that determines the wave tail of the steep wave shock voltage waveform. The potential of is shifted. The low voltage side of the main discharge circuit is then fed back from the low voltage terminal D of the discharge resistor to the low voltage terminal I of the main capacitor through the low voltage connection bar F. Output terminal B is a test object connection terminal when performing a steep wave impact voltage test. The pulse transmission coil L is a series multistage ball gap.
When G 1 ...G o is in a discharging operation, the potential of the main capacitor C changes, but it has a high impedance against steep waves and measures a high withstand voltage.
従つて、本発明に係る急峻波発生装置は放電時
間の遅れ、、放電のばらつきの少ないしかも任意
に遅延制御したトリガーパルスを入れても安定放
電が得られ、始動特性の幅のある著しく向上した
ものとなる。そしてこの種の直列多段球間隙は半
球電極Q、コンデンサC、中間接続電極Wを積み
上げて、容易に高電圧化が行なえる。急峻波衝撃
電圧試験において、本発明に係る急峻波発生装置
を使用すると、放電時間の遅れ、放電のばらつき
が非常に少なくしかも高電圧の安定した急峻波衝
撃電圧波形を被試験物に印加することができる。 Therefore, the steep wave generator according to the present invention has a delay in discharge time, a stable discharge with little variation in discharge, even when a trigger pulse whose delay is controlled arbitrarily is input, and a significantly improved starting characteristic with a wide range. Become something. In this type of series multi-sphere gap, a hemispherical electrode Q, a capacitor C, and an intermediate connection electrode W can be stacked to easily increase the voltage. When the steep wave generator according to the present invention is used in a steep wave shock voltage test, a stable steep wave shock voltage waveform of high voltage can be applied to the test object with very little delay in discharge time and variation in discharge. I can do it.
第3図は急峻波発生装置の組立配置例を示す。
(第2図の回路図に示したものと同一名称のもの
は同一記号を付す。)
主コンデンサ部は絶縁材料からなる枠7,8,
9,10(第3図中枠9は枠8、枠10は枠7の
裏側の位置に配置)の4本で枠組し、その中に主
コンデンサCを配置し、絶縁台17の上に配置す
る。主コンデンサCの上部には蓋板を兼ねた充電
端子TR1で枠組を行ない、主コンデンサCの下部
には主コンデンサ低圧端子Iが接続される。充電
端子TR1と主コンデンサCの低圧端子Iはそれぞ
れ主コンデンサCに電気的に接続されている。直
列多段球間隙部は絶縁材料からなる枠3,4,
5,6と高圧端子Aを兼ねた高圧枠金具と出力端
子Bを兼ねた枠金具で、枠組された内部に形成さ
れている。11および12は半球電極Q31…Qo1を中
間接続電極W1、W2…W(o-1)で固定支持している
絶縁材料からなる固定棒、21および22は半球電
極Q1、Q22…Qo2を中間電極WS1、WS2…Wsoで固
定支持している絶縁材料からなる支持棒である。
また固定棒11および12は高圧端子Aを兼ねた高
圧枠金具と出力端子Bを兼ねた枠金具に固定支持
している。半球電極Q(o+1)1は高圧端子Aに電気的
接続も兼ねて固定支持している。コンデンサC11,
C12 C1(o-2)は各半球電極Q31、Q51…Q(o-1)1より導
出されている中間接続電極W1、W3…W(o-2)の各
間で固定され電気的にも接続されている。コンデ
ンサC21、C22…C2(o-2)も各半球電極W2…W(o-3)、
W(o-1)の各間で固定し電気的にも接続されてい
る。またコンデンサC1(o-2)およびC2(o-2)は高圧端
子Aに電気的接続も兼ねて固定指示し、コンデン
サC11およびC21は出力端子Bに電気的接続も兼ね
て固定支持されている。21は半球電極Q21の絶
縁支持板であり、固定棒12にも固定されている。
19は球間隙調整器で、これを操作することによ
り支持棒21および22が同時に左右に動き、球間
隙G1、G2…Goを同時に調整できる。球間隙G1,
G2…Goの長さは主コンデンサCの充電電圧に応
じて球間隙調整器19により適当に調整される。 FIG. 3 shows an example of the assembly and arrangement of the steep wave generator.
(Those with the same name as those shown in the circuit diagram in Figure 2 are given the same symbol.) The main capacitor part consists of frames 7, 8 made of insulating material,
9 and 10 (frame 9 in Figure 3 is placed on the back side of frame 8 and frame 10 on the back side of frame 7), the main capacitor C is placed in it, and placed on the insulating stand 17. do. The upper part of the main capacitor C is framed by a charging terminal T R1 which also serves as a cover plate, and the lower part of the main capacitor C is connected to the main capacitor low voltage terminal I. The charging terminal T R1 and the low voltage terminal I of the main capacitor C are electrically connected to the main capacitor C, respectively. The series multistage ball gap portion is made of insulating material frames 3, 4,
5 and 6, a high-voltage frame fitting that also serves as the high-voltage terminal A, and a frame fitting that also serves as the output terminal B, and are formed inside the frame. 1 1 and 1 2 are fixed rods made of insulating material that fixedly support hemispherical electrodes Q 31 ...Q o1 with intermediate connection electrodes W 1 , W 2 ...W (o-1) , 2 1 and 2 2 are hemispherical electrodes This is a support rod made of an insulating material that fixedly supports Q 1 , Q 22 ...Q o2 with intermediate electrodes W S1 , W S2 ... W so .
Further, the fixing rods 1 1 and 1 2 are fixedly supported by a high voltage frame metal fitting that also serves as a high voltage terminal A and a frame metal fitting that also serves as an output terminal B. The hemispherical electrode Q (o+1)1 is fixedly supported on the high-voltage terminal A and also serves as an electrical connection. Capacitor C 11 ,
C 12 C 1(o-2) is between each intermediate connection electrode W 1 , W 3 ...W (o-2) derived from each hemisphere electrode Q 31 , Q 51 ...Q (o-1 )1. Fixed and electrically connected. Capacitors C 21 , C 22 ...C 2 (o-2) and each hemispherical electrode W 2 ...W (o-3) ,
It is fixed and electrically connected between each of W (o-1) . In addition, capacitors C 1 (o-2) and C 2 (o-2) are fixed to high voltage terminal A, which also serves as electrical connections, and capacitors C 11 and C 21 are fixed to output terminal B, which also serves as electrical connections. Supported. 21 is an insulating support plate for the hemispherical electrode Q21 , which is also fixed to the fixing rod 12 .
Reference numeral 19 denotes a ball gap adjuster, and by operating this, the support rods 2 1 and 2 2 simultaneously move left and right, allowing the ball gaps G 1 , G 2 . . . G o to be adjusted simultaneously. Gap between spheres G 1 ,
The length of G 2 ...G o is appropriately adjusted by the ball gap adjuster 19 according to the charging voltage of the main capacitor C.
半球電極Q21とQ22,Q31とQ32…Qo1ととQo2は
それぞれ可撓リード板により電気的に接続してい
る。 Hemispherical electrodes Q 21 and Q 22 , Q 31 and Q 32 . . . Q o1 and Q o2 are electrically connected by flexible lead plates, respectively.
絶縁材料からなる枠11,12,13,14
(第3図中枠13は枠12、枠14は枠11の裏
側の位置に配置されている。)の4本で枠組し、
外側に放電抵抗Rを配置し取付けられている。ま
た内側には絶縁材料からなる中空支持筒に同軸ケ
ーブルを巻き付けコイル状に形成したパルス伝送
用コイルLが配置されている。 Frames 11, 12, 13, 14 made of insulating material
(In Figure 3, the frame 13 is placed on the back side of the frame 12, and the frame 14 is placed on the back side of the frame 11.)
A discharge resistor R is placed and attached on the outside. Further, on the inside, a pulse transmission coil L is arranged, which is formed by winding a coaxial cable around a hollow support cylinder made of an insulating material and forming it into a coil shape.
放電抵抗Rの高圧部は出力端子Bを兼ねた枠金
具に固定支持し電気的にも接続され、放電抵抗低
圧端子Dは低圧結線バーRと結線されている。低
圧結線バーFは主コンデンサ低圧端子Iにも結線
され、低圧側の主放電回路を形成している。低圧
結線バーFの配置は接地端子20を兼ねた台座よ
り絶縁台17および18で電気的に絶縁され、電
圧測定上ノイズ対策を考慮したものである。接地
端子20を兼ねた台座の上に前述した主コンデン
サ部、パルス伝送用コイル部、放電抵抗部が配置
される。 The high-voltage part of the discharge resistor R is fixedly supported and electrically connected to a metal frame that also serves as an output terminal B, and the low-voltage terminal D of the discharge resistor is connected to the low-voltage connection bar R. The low voltage connection bar F is also connected to the main capacitor low voltage terminal I, forming a main discharge circuit on the low voltage side. The low-voltage connection bar F is arranged so that it is electrically insulated from the pedestal that also serves as the ground terminal 20 by insulating stands 17 and 18, taking noise countermeasures into consideration when measuring voltage. The above-described main capacitor section, pulse transmission coil section, and discharge resistor section are arranged on a pedestal that also serves as the ground terminal 20.
また主コンデンサ部(主コンデンサCの蓋板を
兼ねた充電端子TR1)の上に絶縁台16を取付
け、さらにその上に多段球間隙部の高圧端子A側
が配置され、枠3,4,5,6が固定支持されて
いる。 In addition, an insulating stand 16 is installed on the main capacitor part (the charging terminal T R1 which also serves as the cover plate of the main capacitor C), and the high voltage terminal A side of the multi-stage ball gap is placed on top of the insulating stand 16, and the frames 3, 4, 5 , 6 are fixedly supported.
多段球間隙部の出力端子B側は放電抵抗Rを取
付けてい枠11…14で枠組みしたものと固定支
持されている
主コンデンサ充電端子TR1と高圧端子Aとはリ
ード線で電気的に接続されている。 The discharge resistor R is attached to the output terminal B side of the multi-stage bulb gap and is fixedly supported by a frame framed by frames 11...14.The main capacitor charging terminal T R1 and the high voltage terminal A are electrically connected with a lead wire. ing.
以上の構造の急峻波発生装置により第2図に示
す回路図が実現でき、前述したような始動特性の
著しく改善した操作に幅のある、しかも従来では
出せなかつた高電圧および安定した確実な急峻波
衝撃電圧が得られる。そして上述の実施例にもと
づいて球間隙15段の急峻波発生装置を製作し、
出力電圧2000KV、急峻波衝撃電圧波形、波頭長
180ns、波尾長1μsが得られた。 The circuit diagram shown in Figure 2 can be realized by the steep wave generator with the above structure, and it has significantly improved starting characteristics as described above, a wide range of operation, high voltage that could not be produced conventionally, and stable and reliable steep wave generation. A wave shock voltage is obtained. Then, based on the above-mentioned embodiment, a steep wave generator with 15 stages of ball gaps was manufactured,
Output voltage 2000KV, steep wave shock voltage waveform, wavefront length
A wave length of 180 ns and a wave tail length of 1 μs were obtained.
また放電のばらつきは30ns以下の安定度が得ら
れた。 Furthermore, the stability of discharge variation was less than 30 ns.
以上詳述のごとく本発明に係る急峻波発生装置
は始動特性を大幅に改善し、かつ安定した高出力
が得られ、工業的ならびに実用的価値の極めて高
いものである。 As described in detail above, the steep wave generator according to the present invention has significantly improved starting characteristics and stable high output, and is of extremely high industrial and practical value.
第1図は従来の球間隙1段の急峻波衝撃電圧発
生装置の回路図、第2図は本発明の急峻波衝撃電
圧発生装置の一実施例の回路図、第3図は本発明
の急峻波衝撃電圧発生装置の配置例で、イは正面
図、ロは側面図である。
C:主コンデンサ、C11,C12……C1(o-2)、C21
C22……C2(o-2):分圧用コンデンサ、G1,G2ー
Go:球間隙、L:パルス伝送コイル、Q22:トリ
ガー電極の絶縁針端付半球電極。
Fig. 1 is a circuit diagram of a conventional steep wave shock voltage generator with one stage of ball gap, Fig. 2 is a circuit diagram of an embodiment of the steep wave shock voltage generator of the present invention, and Fig. 3 is a circuit diagram of a steep wave shock voltage generator of the present invention. An example of the arrangement of a wave impact voltage generator, where A is a front view and B is a side view. C: Main capacitor, C11 , C12 ...C1 (o-2) , C21
C 22 ...C 2(o-2) : Voltage dividing capacitor, G 1 , G 2-
G o : Spherical gap, L : Pulse transmission coil, Q 22 : Hemispherical electrode with insulated needle end of trigger electrode.
Claims (1)
各々の球間〓間電圧が等しくなるように分圧用コ
ンデンサを上記球間〓に互い違いに並列結線する
とともに、主コンデンサに充電された高電圧を、
上記球間〓に設けたトリガー電極にトリガーパル
スを印加することにより球間〓を順次短絡させ、
上記直列多段に結線した球間〓を通じて放電する
急峻波衝撃電圧発生装置において、上記直列多段
に結線した球間〓の出力側に、同軸ケーブルをコ
イル状に形成したパルス伝送コイルを配設し、該
パルス伝送コイルを通じてトリガーパルスを印加
することを特徴とする急峻波衝撃電圧発生装置。1 Connect multiple sets of bulbs in series in multiple stages, and connect voltage dividing capacitors alternately in parallel between the bulbs so that the voltage between each bulb is equal, and connect the high voltage charged in the main capacitor in parallel. voltage,
By applying a trigger pulse to the trigger electrode provided between the spheres, the spheres are successively short-circuited,
In the steep wave shock voltage generator that discharges electricity through the bulbs connected in multiple stages in series, a pulse transmission coil made of a coaxial cable formed into a coil is disposed on the output side of the bulbs connected in multiple stages in series, A steep wave impulse voltage generator characterized in that a trigger pulse is applied through the pulse transmission coil.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3427482A JPS58151880A (en) | 1982-03-03 | 1982-03-03 | Generator for steep-wave impulse voltage |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3427482A JPS58151880A (en) | 1982-03-03 | 1982-03-03 | Generator for steep-wave impulse voltage |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58151880A JPS58151880A (en) | 1983-09-09 |
| JPH0413951B2 true JPH0413951B2 (en) | 1992-03-11 |
Family
ID=12409579
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3427482A Granted JPS58151880A (en) | 1982-03-03 | 1982-03-03 | Generator for steep-wave impulse voltage |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58151880A (en) |
-
1982
- 1982-03-03 JP JP3427482A patent/JPS58151880A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58151880A (en) | 1983-09-09 |
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