• Title/Summary/Keyword: Pulse generator

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Fast Rise Time High Voltage Pulse Generator Applying The Marx Generator (Marx 펄스발생기를 응용한 소형 고전압 급준 펄스 발생장치)

  • Park, Seung-Lok;Chung, Suk-Hwan;Kim, Jin-Gyu;Moon, Jae-Duk
    • The Transactions of the Korean Institute of Electrical Engineers C
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    • v.50 no.2
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    • pp.72-78
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    • 2001
  • A compact size high voltage pulse generator with nanosecond rise time has been designed and investigated experimentally. The inductance of a pulse generator can be reduced by fixing the Marx generator and pulse forming network components into a single cylindrical unit. As a result, nanosecond rise time about $8{\sim}10[ns]$ and pulse width of several hundred [ns] can be obtained from a modified Marx pulse generator. And parametric studies showed that the rise time of the output pulse was depended little on the change of the load resistance and the charging capacitance while, the pulse width of the output pulse was depended greatly upon the change of the load resistance and the charging capacitance. The theoretical showed the possibility to design the laboratory-size pulse generator very fast rising time and a proper pulse width by minimizing stray inductance and varying resistance and capacitance.

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A Damped Sinusoidal Electromagnetic Pulse Generator using a Charged Line (충전선로를 이용한 Damped Sinusoidal 전자기펄스 발생장치)

  • Ryu, Ji-Heon
    • Journal of the Korea Institute of Military Science and Technology
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    • v.9 no.2 s.25
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    • pp.136-142
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    • 2006
  • A damped sinusoidal electromagnetic pulse generator was designed, fabricated and tested. The pulse generator consisted of an oscillator(a spark gap switch and an initially charged low impedance line) and a high impedance antenna. This generator was capable of producing damped sinusoidal pulses at closure of the spark gap switch. A Marx generator was employed to supply the Pulse generator with high voltage pulses. While the pulse generator was provided with the high voltage pulses of 200kV from the Marx generator, its output power was maximized by controlling the pressure of the gas contained in the spark gap switch. The output power of the damped sinusoidal electromagnetic pulse oscillator was 1.3GW and the amplitude of electric field radiated from the pulse generator was 4kV/m at the range of 25m.

Analysis of Output Pulse of High Voltage and Nanosecond Blumlein Pulse Generator

  • Roh, Young-Su;Jin, Yun-Sik
    • Journal of Electrical Engineering and Technology
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    • v.8 no.1
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    • pp.150-155
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    • 2013
  • A high voltage and nanosecond Blumlein pulse generator has been developed to produce an output pulse whose voltage level is greater than 250 kV and pulse duration 5 ns. The generator consists of various components such as a charging circuit, a pulse transformer, and a spark gap switch. As a heart of the generator, a Blumlein pulse forming line has been constructed in the cylindrical form using three cylindrical aluminum electrodes that are placed concentrically. Unlike the ideal Blumlein line, the output pulse of an actual Blumlein line may be affected by stray inductances and capacitances of switching and charging components, thereby degrading the performance of the generator. In this paper, PSPICE simulations have been performed to examine effects of stray inductances and capacitances on waveforms of output pulses. Simulation results show that the pulse waveform is significantly distorted mainly by the stray inductance of the spark gap switch.

A Study on the Pulse Peak Voltage and Cascading Ratio of Compact Pulse Generator using Cascading Method (Cascading 방식을 적용한 펄스발생기의 펄스전압 변성 및 Cascading 비율 특성)

  • Joung, Jong-Han;Kim, Hee-Je
    • The Transactions of the Korean Institute of Electrical Engineers C
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    • v.50 no.7
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    • pp.329-333
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    • 2001
  • The pulsed poser system has been widely used to many applications, such as E/P(Electrostatic Precipitator), DeNox/DeSOx power system, ozon generator, etc. A pulse energy efficiency for load depends on the rising time, peak value, pulse duration and impedance matching, etc. The pulse generator generally required for short pusle duration and high peak value was forced to consider its volume and economy. In this study, developing a compact pulse generator that applied for cascading method to be made of two pulse transformers, we compared cascading voltage with non cascading one by applying the pulse energy to load. Adopting cascading technique to pulse transformer, we found that average cascading voltage was about 60[%] of theoretical value. Maximum cascading ratio was calculated at 60 times compared with non cascading voltage.

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A Study on the Pulse Generator using PFN (PFN을 이용한 펄스발생기의 연구)

  • Lee, B.H.;Joung, K.M.;Park, J.S.
    • Proceedings of the KIEE Conference
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    • 1998.07e
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    • pp.1773-1775
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    • 1998
  • This paper deals with the pulse generator using PFN(Pulse Forming Network), and its operation characteristics and application. Two kinds of pulse generator were composed of the best appropriate condition circuit. The output current of the one pulse generator has the rise time of 28 ns and the pulse duration of $7{\mu}s$. The other pulse generator has high current of about 2kA. By use of the former generator with rapid rise time, the impulse impedance characteristic of ground electrodes was investigated with measuring the ground potential rise when the pulse current was injected into the ground electrode.

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High Efficiency Ozone Generation Using a Pyramid-Project-Embossed Rod-to-Cylinder Electrode and a Pulse Corona Discharge (도깨비봉형 오존발생장치이 펄스커로나 방전에 의한 오존 발생 특성)

  • 문재덕;이근택
    • The Transactions of the Korean Institute of Electrical Engineers
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    • v.38 no.8
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    • pp.650-657
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    • 1989
  • The conversion efficiency of an ozone generator can be significantly improved by modifying the discharge electrode of a helical strip line rod-to-cylinder type ozone generator to a pyramid-project-embossed rod, and by using a pulse corona discharge. Parametric studies have been carried out to obtain optimum values of peak pulse voltage, pulse forming capacitance, feeder cable and ozone generator capacitance, interelectrode spacing and corona tip density of ozone generator, and feed air flow rate and temperature. The generated ozone concentration was very dependent upon the value of pulse forming capacitance, feeder cable and ozone generator capacitance, and corona tip density. Maximum conversion efficiency was obtained with a pulse forming capacitance of about 500pF, 75pF matched feeder cable and ozone generator, and a corona tip density of 16mm. When operated at optimum values, ozone yield of 79, 99, 80 g/KWh for the different interelectrode type ozone generators tested were obtained, which are approximately 30% higher than that of an industrial ozone generator.

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A High Voltage Pulse Generator Using a Rotatary Airhole Spark Gap Code (회전 공극형 고전압 펄스발생장치)

  • 문재덕;이종훈;이복희
    • The Transactions of the Korean Institute of Electrical Engineers C
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    • v.53 no.5
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    • pp.268-272
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    • 2004
  • A high voltage pulse generator with a rotator airhole spark gap instead of a rotary ball spark gap has been proposed and investigated. Its feasibility as a high voltage pulse generator is compared with the rotary ball spark gap type one. Parametric studies showed that proposed the rotary airhole type spark gap had a very stable breakdown voltage and reliable pulse repetition time compared with the conventional rotary ball type spark gap. This however showed that the proposed pulse generator with a rotary airhole spark gap instead of a rotary ball spark gap could be potentially used as a very stable and reliable pulse generator in the various fields of applications.

Compact Size Nanosecond Rise Time Hgh Voltage Pulse Generator (소형 나노초 입상 고전압 펄스발생장치)

  • Park, Sung-Lok;Moon, Jae-Duk
    • Proceedings of the KIEE Conference
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    • 1996.07c
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    • pp.1819-1821
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    • 1996
  • A compact size high voltage pulse generator with nanosecond rise time has been fabricated and investigated experimentally. It can be reduced the inductance of the generator by fixing the Marx generator components and pulse forming network components into a single cylindrical unit. As a result, it can be obtained nanosecond rise time about $8{\sim}10[ns]$ and pulse width of several hundred nanoseconds from the modified Marx pulse generator. And parametric studies showed that the rise time of the output pulse was depended little on the change of the load resister and the charging capacitor while the pulse width of the output pulse was depended greatly upon the change of the load resistor and the charging capacitor.

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Research on the Variable-Width and Double-Pulse Generator (가변폭 Double-Pulse Generator에 관한 연구)

  • 이병선
    • Journal of the Korean Institute of Telematics and Electronics
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    • v.7 no.4
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    • pp.6-13
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    • 1970
  • The variable-width and double-pulse generator Here described is completely transistorized so its size is small and it is convenient to handle. The frequency ran be varied from 1 KHz to 500KHz, the pulse width from 0.4$\mu$sec to 8$\mu$sec, amplitude from 1V to 10V, and interval of double pulse from 0$\mu$sec to 12$\mu$sec. Positive and negative signal or double pulse trains can he obtained. An analysis has been carried out for each stage and the design equations are derived. The experimental results are compared with the analysis.

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Pulse Generator Using Series-Connected Boost Converter (승압형 컨버터의 직렬 배열에 의한 펄스전압 발생회로)

  • 백주원;유동욱;김태진;류명효;조기연;김흥근
    • The Transactions of the Korean Institute of Electrical Engineers B
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    • v.52 no.4
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    • pp.170-176
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    • 2003
  • This paper introduces an improved pulse generator using power semiconductors and L-C circuit. The proposed circuit consists of the series connected boost converter structure. In the presented circuits, high voltage pulse is generated by series-connection of capacitors and IGBTs. The charging of capacitors and voltage balance of IGBTs are obtained automatically. To verify the proposed circuit, 1.8㎸, 40A pulse generator is manufactured and tested.