JPS5883590A - Pulse high voltage generator - Google Patents
Pulse high voltage generatorInfo
- Publication number
- JPS5883590A JPS5883590A JP17869681A JP17869681A JPS5883590A JP S5883590 A JPS5883590 A JP S5883590A JP 17869681 A JP17869681 A JP 17869681A JP 17869681 A JP17869681 A JP 17869681A JP S5883590 A JPS5883590 A JP S5883590A
- Authority
- JP
- Japan
- Prior art keywords
- pulse
- voltage generator
- high voltage
- line
- forming
- 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
Links
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
Landscapes
- X-Ray Techniques (AREA)
- Generation Of Surge Voltage And Current (AREA)
Abstract
Description
【発明の詳細な説明】 を採用したパルス高電圧発生装置に関するものである。[Detailed description of the invention] The present invention relates to a pulse high voltage generator that employs the following.
パルス高電圧発生装着は、従来より比較的小容1の装置
として、パルスX線発生装置や、相対論的電子ビーム発
生装置などに使用されてきた。Pulsed high voltage generators have conventionally been used as relatively small-sized devices in pulsed X-ray generators, relativistic electron beam generators, and the like.
しかし、従来のパルスX線発生のための高電圧電源部は
、マルクス回路を用いた多段式インパルス電圧発生器よ
りなり、面接X線放出部であるダるオードへ電圧を印加
していたため、マルクス回路の回路定数とダイオードの
インピーダンスとによれ決まる放電波形は、例えば第1
図(イ)のような波尾の長いもの、また(ロ)のように
、三角波的な電圧波形であった。However, the conventional high-voltage power supply unit for pulsed X-ray generation consists of a multistage impulse voltage generator using a Marx circuit, and applies voltage to a diode, which is a surface X-ray emitting unit. The discharge waveform determined by the circuit constants of the circuit and the impedance of the diode is, for example, the first
The voltage waveforms were those with long tails as shown in figure (a), and triangular waveforms as shown in figure (b).
そのためXSS形影は、物体が動いている場合、(イ)
ではX線がダラダラと放出されぼける現象があり、(ロ
)ではパルス幅が三角波的であることからX線放出時間
が有効でなく、より高電圧を必要とするなどの欠点があ
った。またX線回折にいたっては、有効なエネルギーの
吸収ができないなどの欠陥があり、fIIJ1図(/つ
のよう碌矩形波の高電圧発生装置の出現が望まれていた
。Therefore, when the object is moving, the XSS shape shadow is (a)
In (b), the X-rays are emitted slowly and become blurred, and in (b), the pulse width is triangular wave-like, so the X-ray emission time is not effective and a higher voltage is required. Furthermore, X-ray diffraction has drawbacks such as the inability to absorb effective energy, and it has been hoped that a high-voltage generator capable of producing a square wave such as fIIJ1 (/) could be developed.
さて、この種のパルス電圧を矩形波に波形成形する試み
としては、相−討論的電子ピ〜ム発生装駿やイオンビー
ム発生装置の例がある。第2図にこれらの従来のパルス
高電圧発生装置、の例を示す。Now, as an attempt to shape this kind of pulse voltage into a rectangular wave, there are examples of a phase-determined electronic beam generator and an ion beam generator. FIG. 2 shows an example of these conventional pulse high voltage generators.
この場合の動作原理を簡単に説明する。マルクス回路を
用いた多段式イン)’< /l/l/スミ生器1は、通
常高電圧を発生することから油絶縁されている。The operating principle in this case will be briefly explained. The multi-stage insulator using a Marx circuit)'< /l/l/The Sumie generator 1 is usually oil-insulated because it generates a high voltage.
2は金属で作られた同軸状の波形成形線路の一部を示し
たもので、誘電体にはインピーダンスの値によって異な
るが、油、水、S F gガスなどが用いられる。そQ
M路の長さは必要とするパルス幅によって決定される。2 shows a part of a coaxial waveform-shaped line made of metal, and the dielectric material used is oil, water, S F g gas, etc., depending on the impedance value. SoQ
The length of the M path is determined by the required pulse width.
3は絶縁容器、に収容されたガス充填形の主放電スイ咋
チ、4け真空室に配置されたγノードとカソードからな
る2極のダイオード部で、電極の形状については説明を
しないが、MTh性の場合は電子ビームを、正極性の場
合はイオンビームを放出する。動作はインパルス電圧発
生器1を適正に制御されたトリガーパルサーにより放−
させ、その電荷を一旦波形成形線#62に蓄え、その電
圧が最大値付近に達すると、適正に圧力調整された主放
電スイッチ3が自爆動作して、パルス伝送りイン5を経
てダイオード4に進行波理論に基づくところの矩形波が
伝送される。なお波形成形線路2、パルス伝送りイン5
の各々のインピーダンスは通常ダイオード4と同一値に
設計され、インピーダンスマヴチングがとられているた
め、ダイオード4には理想的には波形成形線路2の充電
電圧の半分の電圧が供給されることになる。このように
波形成形については、すでに実用化されているが、一般
的に大エネルギーの装置、例えば加速電圧(1〜5 )
MeV、 エネルギー(10〜200)KJ、 パ
ルス幅(50〜100)is などに使用されており
、低エネルギーの装置であるパルスX纏装瞳、例えば加
速電圧(01〜1 )MeV、 エネルギー((1,
01〜1 )KJ、 パルス@(10〜30)111
度に使用するには構造的にも大型となり、かつ低インピ
ーダンスの場合パルス成形線路の内外径比が小さくなる
ことがら電界強度を適正値にre定するとどうしても直
径の大きなものとなり、無効体積分を多く有することな
どポリコーム的にも好ましくない形状となる欠点があっ
た。3 is a gas-filled main discharge switch housed in an insulating container, and a two-pole diode section consisting of a γ node and a cathode placed in a four-chamber vacuum chamber.The shape of the electrodes will not be explained here, but An electron beam is emitted when the polarity is MTh, and an ion beam is emitted when the polarity is positive. In operation, the impulse voltage generator 1 is released by a properly controlled trigger pulser.
Once the charge is stored in the waveform forming line #62, and the voltage reaches around the maximum value, the main discharge switch 3, whose pressure has been properly adjusted, self-destructs, and the electric charge is transferred to the diode 4 via the pulse transmission line 5. A rectangular wave based on traveling wave theory is transmitted. In addition, waveform shaping line 2, pulse transmission line 5
The impedance of each is normally designed to have the same value as the diode 4, and impedance machining is performed, so ideally a voltage half the charging voltage of the waveform shaping line 2 is supplied to the diode 4. Become. Although waveform shaping has already been put into practical use, it is generally not possible to use large energy devices such as accelerating voltage (1 to 5).
It is used for MeV, energy (10-200) KJ, pulse width (50-100) is, etc., and is used for pulse 1,
01-1) KJ, Pulse @ (10-30) 111
It is structurally large to be used frequently, and in the case of low impedance, the ratio of the inner and outer diameters of the pulse shaping line becomes small, so if the electric field strength is set to an appropriate value, the diameter will inevitably become large, and the ineffective volume will be reduced. There is a drawback that having a large amount of polycomb results in an unfavorable shape.
本発明は上記の欠点を除去し、小型で経済性に富み、力
tつ性能の優れたパルス高電圧発生装置を提供しようと
するものである。The present invention aims to eliminate the above-mentioned drawbacks and provide a pulsed high voltage generator that is compact, economical, and has excellent power and performance.
以下、本発明を第3図〜第5図に示す実施例について説
明する。The present invention will be described below with reference to embodiments shown in FIGS. 3 to 5.
第3図は本発明のパルス高電圧発生装置の要部断面図、
第4図はその等価回略図で、マルクス回路を用いた多段
式インパルス発生器は5段の例である。6け高圧側充電
抵抗、6′は低圧側充電抵抗で、各5個直列に接続され
ている。7はコンデンサ、8は最下段のトリがトロン形
成Wスイ呼チ、8′は自爆式放電スイッチ、9は零宛叫
の主目的である多段式゛インパルス電圧発生器の外周を
覆いがふせるように配置した導電性の内鯛の筒、1oは
全ての機器を収納する導電性の外側の筒で、この筒9と
fllloが同軸状に配着され、両筒9,10間の静電
容tllbとインダクタンス11&によってインピーダ
ンスが決定され、かつその長さでパルス幅が決まる。す
なわち、筒9と筒10によって第4図に示すような分布
定数回路を有する波形成形線路11が形昨される。12
は主放電スイッチ、13は真空容器内の負荷側のダイオ
ード14にパルス電圧を伝播するパルスライン、】5は
主放電スイッチ12の圧力容器であり、かつ真空室16
を有し、高圧発生器としての高圧出カブ9シングでもあ
る。17はインパルス電圧発生器の各種部品を締付ける
ための絶綽棒、18は放電抵抗、19は油、SFaガス
など目的により選択される絶縁体である。FIG. 3 is a sectional view of the main parts of the pulsed high voltage generator of the present invention,
FIG. 4 is an equivalent circuit diagram thereof, and is an example of a five-stage multistage impulse generator using a Marx circuit. 6 high-voltage side charging resistors, 6' is a low-voltage side charging resistor, and 5 of each are connected in series. 7 is a capacitor, 8 is the lowest bird that forms a tron W switch, 8' is a self-destruct discharge switch, and 9 is a multi-stage "impulse voltage generator" whose main purpose is to cover the outer periphery of the impulse voltage generator. The conductive inner tube 1o is a conductive outer tube that houses all the equipment, and this tube 9 and flllo are arranged coaxially, and the capacitance tllb between the two tubes 9 and 10 is The impedance is determined by the inductance 11&, and the pulse width is determined by the length thereof. That is, a waveform shaping line 11 having a distributed constant circuit as shown in FIG. 4 is formed by the cylinder 9 and cylinder 10. 12
13 is a pulse line that propagates a pulse voltage to a diode 14 on the load side in the vacuum vessel; 5 is a pressure vessel for the main discharge switch 12;
It is also a high pressure output unit as a high pressure generator. Reference numeral 17 is a bolt for tightening various parts of the impulse voltage generator, reference numeral 18 is a discharge resistor, and reference numeral 19 is an insulator selected depending on the purpose, such as oil or SFa gas.
次にその動作を説明するg
直流高電圧発生器2(lより充電抵抗6.6′、放電抵
抗18 t−aして、各コンデンサ7を並列に充電した
後、最下段のトリガトロン形放電スイッチ8に適正に制
御され九トリガーパルスを与える。これにより放電スイ
ッチ8が放電し、他の放電スイッチ8′も股間、の分布
容量と対地間容量の静電分圧に29生じた過電圧により
、下段よりつぎつぎと自爆放電し、やがて全段直列放電
して波形成形線路IIを構成している同軸状の導電性筒
9と10の間の同軸コンデンサを充電することになる。Next, we will explain its operation.g DC high voltage generator 2 (from l, charging resistor 6.6', discharging resistor 18 t-a, after charging each capacitor 7 in parallel, the lowest stage triggertron type discharge Appropriately controlled trigger pulses are given to the switch 8. This discharges the discharge switch 8, and the other discharge switch 8' also discharges due to the overvoltage generated in the electrostatic partial pressure of the distributed capacitance between the crotch and the ground capacitance. Self-destructive discharge occurs one after another from the lower stage, and eventually all stages are discharged in series to charge the coaxial capacitor between the coaxial conductive cylinders 9 and 10 forming the waveform forming line II.
この電圧が最大値に達すると、適正に調整された主放電
スイッチ12が自爆wJ作し、前記波形成形線路11す
なわち同軸状の導1[性wJ9と10の間に蓄iされた
電荷は、−荷伺のダイオードI4ヘバルスラ、イン13
を経て、進行波理論によるところの矩形波を伝播するこ
とになる。回路定数の選択は目的により異なるが、一般
的には次の通りである。When this voltage reaches its maximum value, the properly adjusted main discharge switch 12 self-destructs, and the charge stored between the waveform-shaped line 11, i.e. the coaxial conductor 1 [wJ9 and 10], is -Loading diode I4 Hebalsura, In13
Through this process, a rectangular wave according to the traveling wave theory is propagated. The selection of circuit constants varies depending on the purpose, but is generally as follows.
> C,・・、・・、、、−四一・曲・・−・・曲・
−・・・曲・・・−・・冊−・・(1)ZL2:ZPF
L・・・・・・・・・・・−・・・・・・・・・・・・
聞−・・・・・・曲用・・曲(2)ただし、
n:マルクス回路の多段式インパルス電圧発生器の段数
C:マルクス回路の単位コンデンサの静電容量co=波
形成形線路の静電容量
ZPFL:、波形成形線路のインピーダンスzL :ダ
イオード部のインピーダンスただし、
rl:導電性筒9の外半径
rl:導電性筒10の内半径
ε:導導電性筒l円内絶縁体の誘電率
以上のように本発明のパルス高電圧発生装置は特に低イ
ンピーダンスになると(3)式より解がるように、内外
径比rz/γ1は小さくなり、しかも同軸円筒の電界強
−2度を考Iする(破壊値以下にする)とどうしてもそ
の直径が大きくなることから、そのパルス成形線路11
を構成する導電性筒9の中は無駄な空間となるので、そ
の中に絶縁空間を適切に設けて多段式インパルス電圧発
生器20を有効に配蓋し、一体化したものである。一方
パルス成形線路を構成する外側の導電性筒10は外装容
器として併用でき、また内側の導電性筒9と外側の導電
性筒10間の静電容量、インダクタンス、そして長さを
適宜選択したり、また場合によっては、絶縁体を油、ガ
スなどの誘電体の異なる本のを使用することにおり、必
要とする矩形波パルスを負荷側のダイオード14に供給
することができる。> C,...,...,, -41・song・---・song・
-... Song... -... Book - (1) ZL2:ZPF
L・・・・・・・・・・・・-・・・・・・・・・・・・
Song - Song (2) Where, n: Number of stages in the multi-stage impulse voltage generator of the Marx circuit C: Capacitance co of unit capacitor in the Marx circuit = Electrostatic capacity of the waveform forming line Capacitance ZPFL: Impedance of the waveform-shaped line zL: Impedance of the diode section, where: rl: Outer radius of the conductive tube 9 rl: Inner radius of the conductive tube 10 ε: More than the dielectric constant of the insulator inside the conductive tube l As can be seen from equation (3), when the pulsed high voltage generator of the present invention has a particularly low impedance, the inner/outer diameter ratio rz/γ1 becomes smaller, and considering the electric field strength of the coaxial cylinder -2 degrees, If the pulse forming line 11 is
Since the inside of the conductive cylinder 9 constituting the casing 9 is a wasted space, an insulating space is appropriately provided therein to effectively enclose the multistage impulse voltage generator 20 and integrate it. On the other hand, the outer conductive tube 10 constituting the pulse forming line can be used as an outer container, and the capacitance, inductance, and length between the inner conductive tube 9 and the outer conductive tube 10 can be selected as appropriate. In some cases, a different type of dielectric material such as oil or gas may be used as the insulator, and the required rectangular wave pulse can be supplied to the diode 14 on the load side.
なお、上述の実施例は、パルス成形線路11を、多段式
インパルス電圧発生器21に結合し、しかも該発生器2
1の外周部に配置し九場合について述べたが、他の方式
のインパルス電圧発生器に結合する場合についても同様
に適用できる。例えば第5図に示すようなパルス変圧器
22を用いた昇圧方式のパルス品電圧発生装置において
も第3図と同様にパルス変圧器22の外周部に同軸状の
41iiC性筒9゜10からなるパルス成形線路11を
関着して結合することにより同様な効果が得られる。こ
9場合の動作は充電スイッチnを閉じて、遊場に制御さ
れた゛直流高圧発生器2()により充電抵抗Uを通して
コンデンサ25を充電する。充電完了後、放電スイ−1
626を閉じると、コンデンサ25の電荷はパルス変圧
fi22へ放出され、その変圧器の2次側へ巻線比に比
例した電圧が発生し、その電圧までインダクタンス11
aと静電容量11 bのnp段等価回路に噴き換え示
したパルス旋形線路】1を充電することになる。以後、
この電圧が最大値に達すると、適正に調整され之王放電
スイ・Iチ12が自爆動作し、上記波形成形線路11に
蓄積された電荷は負荷側のダイオード14へ進行波理論
によるところの矩形波を伝播することになる。It should be noted that the embodiment described above couples the pulse shaping line 11 to a multi-stage impulse voltage generator 21, and the generator 2
Although the case has been described in which the present invention is arranged on the outer periphery of the first impulse voltage generator, the same applies to cases in which it is coupled to impulse voltage generators of other types. For example, in a step-up pulse voltage generator using a pulse transformer 22 as shown in FIG. 5, a coaxial 41iiC cylinder 9° 10 is attached to the outer periphery of the pulse transformer 22 as shown in FIG. A similar effect can be obtained by articulating and coupling the pulse shaping lines 11. The operation in this case is to close the charging switch n and charge the capacitor 25 through the charging resistor U using the DC high voltage generator 2 () controlled by the play field. After charging is complete, discharge switch 1
626, the charge in the capacitor 25 is discharged to the pulse transformer fi22, and a voltage proportional to the winding ratio is generated on the secondary side of the transformer, and up to that voltage, the inductance 11
The pulse spiral line 1 shown in FIG. From then on,
When this voltage reaches the maximum value, it is properly adjusted and the No. 1 discharge switch I switch 12 self-destructs, and the charge accumulated in the waveform shaping line 11 is transferred to the diode 14 on the load side in a rectangular shape according to the traveling wave theory. It will propagate waves.
このように多段式インパルス電圧発生器、もしくはパル
ス変圧器の外周部へ、橿いかぶさるようにパルス成形線
路を設けた一体構造のパルス高電圧発生装置は、容易に
矩形波を得ることができ、かつ小形にでき、第1図のよ
うに独立した波形成形線絡付は方式を結合した別付は方
式の従来品に比し、本発明品は容積で1 / 2.5に
減少し、経済的−にも安価になった。In this way, a multi-stage impulse voltage generator or an integrated pulse high voltage generator in which a pulse shaping line is provided over the outer circumference of a pulse transformer can easily generate a rectangular wave. In addition, it can be made compact, and as shown in Figure 1, compared to the conventional product that combines the independent waveform wire attachment method and the separate attachment method, the volume of the product of the present invention is reduced to 1/2.5, making it more economical. It has also become cheaper.
以上のように本発明のパルス高電圧発生装置は構造、性
能両面において極めて有益となり、パルスX線装置や比
較的小容量の粒子ビーム発生装6電などの高圧電源とし
て工業的ならびに実用的警備の大なるものである −As described above, the pulsed high voltage generator of the present invention is extremely useful in terms of both structure and performance, and is useful for industrial and practical security purposes as a high voltage power source for pulsed X-ray equipment, relatively small capacity particle beam generators, etc. It is a great thing −
第1図は各種パルス高電圧波形図、第2図は従来のパル
ス高電子余生装置の要部切断図、第3図は本発明のパル
ス高電圧発生装置の一実施例の要部切断図、@4図は同
本発明のパルス高電圧発生装置の尋゛価回路図、第5図
は本発明のパルス蒔電圧発生装置の他の賽施例の等何回
略図である。
7.25:コンデンサ
8、8’、12 :放電スイダチ
9、Hl:導電性筒
月:パルス成形線路
】4:負荷側のダイオード
21 : 、8般式インパルス電圧発生器22:パルス
変圧器
特許出願人 日本コンデンサ工業株式会社第1図
<=r )(ニー゛) (7、。
第2図
第3図
第4図
第5図
丁続補市書(自究)
昭和56年12月1011
持占II’ 、1< ’l”; 島 1)春樹 殿1
・Jl(十 〇) 表 小
昭和5611特許願第178696弓
ゴ 1こ明り)8称
パルスil!6電圧発生装眩
3、 h(i +[、: ヲr ルg$(′1との関
係 特ト出願人
市部市中京区御池通烏丸東大・筋目
仲保利町1月計地の4 上絵ヒル3階
[明細書の発明の詳細な説明の楠」および「図面」
5、補正の内容
(1) 明細書第9頁1420行を次のように訂正す
る。
「ンヌ11 aと静電容量11 bの等何回路に置き」
(2) 明#tl*第10頁第月行を次のように訂正
する。
[かつ小形にでき、第2図のようしこ独立した波形成」
(3) 図面の中第3図を別紙のように81′正する
。FIG. 1 is a diagram of various pulsed high voltage waveforms, FIG. 2 is a cutaway diagram of a main part of a conventional pulsed high electron residual device, and FIG. 3 is a cutaway diagram of a main part of an embodiment of a pulsed high voltage generator of the present invention. Figure 4 is a basic circuit diagram of the pulsed high voltage generator of the present invention, and Figure 5 is a schematic diagram of another embodiment of the pulsed high voltage generator of the present invention. 7.25: Capacitor 8, 8', 12: Discharge suidachi 9, Hl: Conductive cylinder: Pulse forming line] 4: Diode on load side 21: , 8 General type impulse voltage generator 22: Pulse transformer patent application Person Nippon Capacitor Industry Co., Ltd. Figure 1 <=r ) (Ni) (7. Figure 2 Figure 3 Figure 4 Figure 5 Supplementary City Paper (self-study) December 1981 1011 Ownership II', 1<'l'; Island 1) Haruki-dono 1
・Jl (10 〇) Table Small Showa 5611 Patent Application No. 178696 Yugo 1 light) 8th pulse il! 6 Voltage generation glare 3, h(i + [,: wo r g $ ('1) Special applicant Oike-dori Karasuma Tokyo University, Nakagyo-ku, Ichibe-shi Hill 3rd Floor [Detailed Explanation of the Invention in the Specification and Drawings] 5. Contents of Amendment (1) Page 9, line 1420 of the specification is corrected as follows: "Nnu 11 a and capacitance 11.What circuit should I put it in, such as b?
(2) Bright #tl* The month line on page 10 is corrected as follows. [And it can be made small, with independent wave formation as shown in Figure 2.'' (3) Figure 3 in the drawing is corrected by 81' as shown in the attached sheet.
Claims (3)
外周部に配置した同軸状の導電性筒からなるパルス成形
線路と、該パルス成形線路と負荷側との間に直列に接続
した放電スイッチとを具備し、上記高電圧発生器の電圧
をパルス成形線路を介して放電することを特徴とするパ
ルス高電圧発生装置。(1) A pulse forming line consisting of a coaxial conductive tube connected to the output end of a high voltage generator and placed on the outer periphery of the generator, and a pulse forming line connected in series between the pulse forming line and the load side. A pulsed high voltage generator, comprising a discharge switch connected to the pulsed high voltage generator, and discharges the voltage of the high voltage generator through a pulse shaping line.
電スイッチなどを積上げてなる多段式インパルス電圧発
生器からなることを特徴とする特許請求の範囲第1項記
載のパルス高電圧発生装着。(2) The pulse high voltage generation device according to claim 1, wherein the high voltage generator is a multistage impulse voltage generator formed by stacking a plurality of capacitors, discharge switches, etc.
ス変圧器の外周部に同軸状の導iI性筒からなるパルス
成形線路を配置したことを特徴とする特許請求の範囲s
i項紀載のパルス高電圧発生装置。(3) Claim s characterized in that the high voltage generator has a pulse transformer, and a pulse shaping line made of a coaxial conductive cylinder is arranged on the outer periphery of the pulse transformer.
Pulse high voltage generator described in Section i.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP17869681A JPS5883590A (en) | 1981-11-07 | 1981-11-07 | Pulse high voltage generator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP17869681A JPS5883590A (en) | 1981-11-07 | 1981-11-07 | Pulse high voltage generator |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5883590A true JPS5883590A (en) | 1983-05-19 |
JPH0161256B2 JPH0161256B2 (en) | 1989-12-27 |
Family
ID=16052947
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP17869681A Granted JPS5883590A (en) | 1981-11-07 | 1981-11-07 | Pulse high voltage generator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5883590A (en) |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01171213A (en) * | 1987-12-25 | 1989-07-06 | Mitsui Petrochem Ind Ltd | Power supply equipment for generating high voltage and highly repetitive pulse |
JPH04120781A (en) * | 1989-12-21 | 1992-04-21 | Hughes Aircraft Co | High-tension power supply |
WO2014013645A1 (en) * | 2012-07-18 | 2014-01-23 | 株式会社リガク | Industrial x-ray generator for non-destructive inspection |
JP2015534342A (en) * | 2012-09-14 | 2015-11-26 | イテアシュぺぺ | A substantially square high power pulse generator with adjustable slope. |
CN108322982A (en) * | 2018-04-12 | 2018-07-24 | 中国工程物理研究院流体物理研究所 | Ferroelectric Explosive electricity transducing impulse generator, flash X-ray generation device and method |
CN109713931A (en) * | 2018-12-06 | 2019-05-03 | 西安交通大学 | Nanosecond rise time Impulsive Current generating device based on vacuum tightness environment |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0527559Y2 (en) * | 1988-02-24 | 1993-07-14 |
-
1981
- 1981-11-07 JP JP17869681A patent/JPS5883590A/en active Granted
Cited By (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01171213A (en) * | 1987-12-25 | 1989-07-06 | Mitsui Petrochem Ind Ltd | Power supply equipment for generating high voltage and highly repetitive pulse |
JPH04120781A (en) * | 1989-12-21 | 1992-04-21 | Hughes Aircraft Co | High-tension power supply |
WO2014013645A1 (en) * | 2012-07-18 | 2014-01-23 | 株式会社リガク | Industrial x-ray generator for non-destructive inspection |
JP2014022185A (en) * | 2012-07-18 | 2014-02-03 | Rigaku Corp | Industrial x-ray generation device for nondestructive inspection |
KR20150031395A (en) | 2012-07-18 | 2015-03-24 | 가부시키가이샤 리가쿠 | Industrial x-ray generator for non-destructive testing |
JP2015534342A (en) * | 2012-09-14 | 2015-11-26 | イテアシュぺぺ | A substantially square high power pulse generator with adjustable slope. |
CN108322982A (en) * | 2018-04-12 | 2018-07-24 | 中国工程物理研究院流体物理研究所 | Ferroelectric Explosive electricity transducing impulse generator, flash X-ray generation device and method |
CN109713931A (en) * | 2018-12-06 | 2019-05-03 | 西安交通大学 | Nanosecond rise time Impulsive Current generating device based on vacuum tightness environment |
CN109713931B (en) * | 2018-12-06 | 2020-05-19 | 西安交通大学 | Nanosecond rise time strong pulse current generating device based on vacuum closed environment |
Also Published As
Publication number | Publication date |
---|---|
JPH0161256B2 (en) | 1989-12-27 |
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