• Title/Summary/Keyword: Fast-rise pulse

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Power Cell-based Pulsed Power Modulator with Fast Rise Times (빠른 상승 시간을 갖는 파워 셀 기반 펄스 파워 모듈레이터)

  • Lee, Seung-Hee;Song, Seung-Ho;Ryoo, Hong-Je
    • The Transactions of the Korean Institute of Power Electronics
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    • v.26 no.1
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    • pp.25-31
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    • 2021
  • This paper describes the design of a power cell-based pulsed power modulator with fast rise times. The pulse-generating section of the pulse power modulator is a series stack of power cells. Each power cell is composed of a storage capacitor, a pulse switch, and a bypass diode. When the pulse switches are turned on, the capacitors are connected in series and the sum of voltages is applied to the load. For output pulses with fast rise times, an IGBT with fast turn-on characteristics is adopted as a pulse switch and the optimized gate driving method is used. Pspice simulation is performed to account for the gate driving method. A 10 kV, 12-power cell-based pulsed power modulator is tested under resistive load and plasma reactor load. The rise times of output pulses less than 20 ns are confirmed, showing that the pulsed power modulator can be effectively applied to pulsed power applications with fast rise times.

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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Sinusoidal A Study on the gain Stability of the Feedback Linear Pulse Amplifiers for Fast Pulse Input (금속펄스 선형증폭기의 빠른 입력펄스에 대한 이득안정도에 관한 연구)

  • 이병선
    • Journal of the Korean Institute of Telematics and Electronics
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    • v.11 no.3
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    • pp.1-14
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    • 1974
  • The gain stability of the nuclear pulse linear amplifiers with feedback for such a fast pulse input as the step voltage or the nuclear radiation detector pulse is analysed in detail. The expression is derived which describes the waveform at the anode circuit of the photomultiplier tube which is a part of the nuclear radiation detector. It is analysed and compared when the feedback amplifier has one and two time-constants. When these fast input pulse voltages are applied to the feedback amplifier, the effects of feedback in linearity and stability of the output voltage appear only after two or three rise-times of the amplifier, And it is proved that in order to reduce this limitation, the rise time of the feedback amplifier shou1d be less than the input pulse width. It is also shown that the above theory can be applied directly to the voltage-shunt feedback amplifier stages designed as the basic amplifier of the linear amplifier, and that the gain stability is more improved for the smaller input impedance of this amplifier stage.

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A System on the Gain Stability of Negative Feedback Pulse Linear Amplifier (부귀환펄스선형증폭기의 이득 안정도에 관한 연구)

  • 이병선
    • Journal of the Korean Institute of Telematics and Electronics
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    • v.10 no.5
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    • pp.7-15
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    • 1973
  • The gain stability of the nuclear pulse ampifiers with negative feedback for such a fast pulse input as the step voltge or the nuclear radiation detector pulse is analyzed in detail and the experimental results are given. It is shown that a few risetime should elapse to get the full effect of the negative feedback upon the liearity and the stability of the amplifiers for the fast pulse input, and to reduce this limitation the risetime of the negative feedback amplifier must be designed to be short compared with the width of the input pulse.

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Comparative Analysis on Ground Impedance for a Carbon Block and a Copper Rod (탄소블록과 동봉의 접지임피던스 비교 분석)

  • Seo, Jae-Suk;Park, Hee-Chul;Kil, Gyung-Suk;Oh, Jae-Geun
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.26 no.6
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    • pp.472-477
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    • 2013
  • This paper carried out the comparative analysis on ground impedance of a carbon block and a copper rod. Two types of grounding electrode were compared ; a carbon block (L : 1 m, ${\Phi}$ : 245 mm) buried at a depth of 0.8 m and a three-linked copper rod (L : 1 m, ${\Phi}$ : 10 mm) of equilateral triangles with 1 m spacing. Ground impedance depending on applied current source was evaluated by the application of a sine wave current with 60 Hz ~ 3.5 MHz, a fast-rise pulse with rising time of 200 ns, a standard lightning impulse of $8/20{\mu}s$ and a 600 Hz square wave. Ground impedance for both electrodes were almost the same value below 100 kHz, and increased rapidly afterwards. The maximum ground impedance appeared $400{\Omega}$ at around 1.5 MHz. Ground impedance of the carbon block was lower at the square wave and was higher at fast-rise pulse than that of the copper rod. Also, ground impedance as ages showed no difference for the last 8 months. From the results, it is likely that ground performance for both electrodes shows no difference against commercial frequency and lightning impulse current, while the copper rod shows better performance against a fast-rise pulse with rise-time of a few hundred ns.

Fabrication of 200kV Coaxial Type Marx Generator and its Performances (200kV급 동축형 Marx 펄스발생장치 제작 및 동작특성)

  • Lee, Sang-Woog;Lee, Chae-Min;Koo, Ja-Yoon;Chang, Yong-Moo
    • Proceedings of the KIEE Conference
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    • 2008.10a
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    • pp.89-90
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    • 2008
  • Pulsed power technologies in variable fields require the pulsed high power sources. We fabricated the pulsed power generator, named EMD Pulse Generator(EPG), by using Marx circuit with 200 kV high, 50 ns fast rise time. In this paper, we described about the performances.

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Compact Pulse Generator Using a Rotating Disk with Sparking Holes (회전공판형 컴펙트 펄스 발생장치)

  • Lee, Jong-Hoon;Kwon, Nam-Yeol;Lee, Seung-Hoon;Shin, Jung-Min;Moon, Jae-Duk
    • Proceedings of the KIEE Conference
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    • 2003.07c
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    • pp.1870-1872
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    • 2003
  • High voltage pulse generator with fast rise time has been studied theoretically and experimentally. The complexity and stray inductance of a pulse generator components can be very difficult to reduce. As a result, a compact size and stable Pulse can be obtained by using a rotary air-hole. Parametric studies showed that the rise time of the output pulse was depended little on the change of the revolutions per minute(RPM) while the pulse width of the output pulse was depended greatly upon the change of the revolutions per minute (RPM).

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Generation of Ultrawide Band Electromagnetic Pulse from Blumlein Pulse Forming Line

  • Jin, Yun Sik;Kim, Jong Soo;Cho, Chuhyun;Roh, Young Su
    • Journal of Electrical Engineering and Technology
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    • v.9 no.2
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    • pp.677-681
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    • 2014
  • A high voltage pulse generator was fabricated to radiate ultrawide band electromagnetic pulse. A coaxial type of Blumlein pulse forming line is employed to produce a pulse of high voltage (>300 kV) and short pulse duration (~5 ns). A helical strip/wire type of air-cored pulse transformer was used to charge the Blumlein pulse forming line up to more than 300 kV. A peaking switch is essential to make the pulse rise time as fast as possible. Typically, the rise time is ~500 ps. The output pulse of the generator is radiated into air through an exponentially tapered TEM horn antenna. The electric field intensity of a radiated pulse was measured as a function of the distance from the transmitting horn as well as the output voltage of the peaking switch. The peak-to-peak value of the electric field intensity at 10 m from the TEM antenna was~100 kV/m.

A STUDY ON THE SELF-MATCHED LINE PULSE GENERATOR (자기정합 선로형 펄스 발생기에 관한 연구)

  • Paek, Yong-Hyun;Sohn, Jae-Hoon
    • Proceedings of the KIEE Conference
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    • 1990.11a
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    • pp.184-187
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    • 1990
  • This paper presents the self-matched line pulse generator and the concerned principles on its operation and characteristics are mentioned. The circuit consists of a charged transmission line and a high speed switch, and it generates a square wave pulse with the very fast rise time. The generated waveform depends on the load resistance. As the load resistance is infinite, a single rectangular wave pulse is generated and its efficiency is nearly unity.

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Coaxial Marx Type Pulse Generator for UWB EM Pulse (UWB 펄스전자파 발생용 원통형 Marx 펄스발생장치개발)

  • Chang, Yong-Moo;Lee, Sang-Wook
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2010.06a
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    • pp.121-121
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    • 2010
  • As the industrial technology is getting higher, the pulsed power technology is required from various fields such as thermonuclear fusion energy sources, military applications, electric power distribution, and a variety of new specialized needs. This technology deals with the generation of very high power electromagnetic pulses through fast switching. We fabricated a pulsed power generator, named EMD pulse generator, by using Marx circuit with 200 kV high, 50 ns fast rise time. In this paper, we described about an effect of stray capacitance of coaxial Marx generator, EPG-AM200k, and a comparing the results of experiments and circuit analysis.

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