• 제목/요약/키워드: discharge plasma

검색결과 1,423건 처리시간 0.026초

대기압 플라즈마 발생시 인가전압의 상승시간에 따른 영향 (Effect of Rise Time of a Pulse Bias Voltage on Atmospheric Plasma Generation)

  • 김재혁;진상일;김영민
    • 전기학회논문지
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    • 제57권7호
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    • pp.1218-1222
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    • 2008
  • We investigate the effect of rise time of a pulse bias voltage on atmospheric plasma generation. With the faster rise time of the pulse bias, the glow discharge appears to be more uniformly generated along the electrodes. I-V measurement confirms that higher loading power can be obtained using the faster rise time. A new understanding for atmospheric plasma generation at a micro-gap electrode is suggested.

Plasma display panels; problems and their analysis via computer simulations

  • Nagorny, V.P.;Khudik, V.N.;Drallos, P.J.;Shvydky, A.
    • 한국정보디스플레이학회:학술대회논문집
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    • 한국정보디스플레이학회 2005년도 International Meeting on Information Displayvol.I
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    • pp.155-160
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    • 2005
  • Computer simulations of a pdp discharges provide unique information necessary for their analysis, unavailable otherwise. Statistical instability of the ramp discharge and the role of exoemission, nature of striations during sustain discharge, physical mechanism responsible for the propagation of the cathode ionization wave, and line loading effects are just a few examples when simulations can be successfully used.

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DBD (Dielectric Barrier Discharge) Plasma Device for Biomedical Applications

  • 김윤중;김중길;정종윤;한국희;이민경;차덕봉;한상호;박경순;조광섭
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2012년도 제42회 동계 정기 학술대회 초록집
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    • pp.461-461
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    • 2012
  • 미생물 처리에 적용하기 위한 저주파 Dielectric Barrier Discharge (DBD) Plasma Device를 고안하였다. 현재 생의학적으로 광범위하게 사용되는 Plasma Jet Device는 가스를 주입해 주어야 한다. 그러나 Plasma Jet Device의 노즐로부터 배출되는 가스는 Media의 흔들림과 증발 유발시키며 미생물에게 영향을 미친다. 가스 배출에 의한 영향을 없애기 위해 가스 주입이 없는 Plasma 발생 장치를 제작 하고, 미생물에 적용하여 그 효과를 관찰하였다. 본 실험에 사용된 Plasma 발생 장치는 대기 중에서 방전된다. 가스의 주입 없이 낮은 방전 전압과 균일한 플라즈마의 발생을 위해 Plasma 발생 장치의 접지 전극으로 Mesh를 사용 하였다. 본 Plasma 발생 장치로 발생된 Plasma를 곰팡이(Fusariumgraminearum)에 조사한 결과, 조사 시간이 길어짐에 따라 배양된 곰팡이의 Colony 수가 Plasma를 조사하지 않은 경우에 비해 줄어드는 것을 확인할 수 있었다. 또한 각각의 곰팡이 Colony의 크기도 줄어들었다.

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수중 스트리머 방전용 플라즈마 반응기 구조에서 수소발생 특성 (The Characteristic of Hydrogen Generation on the Structure of Plasma Reactor Using the Streamer Discharge in the Water)

  • 박재윤;김종석
    • 조명전기설비학회논문지
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    • 제20권4호
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    • pp.37-42
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    • 2006
  • 본 논문에서는$CO_2$를 발생시키지 않고 물로부터 직접 수소를 제조하기 위하여 비열플라즈마를 이용하였다. 다중침-평판형(Multineedle-plate electrode geometry reacto: MPER)과 단일침-평판형(Needle-plate electrode geometry reactor: NPER) 두종류의 수소제조 반응기를 설계 제작하여 수소 발생에 미치는 영향에 대하여 실험하였다. 수소발생을 높이기 위해서는 강한 아크성 스트리머 방전 발생과 효과적인 수표면 방전을 위한 수표면 조건을 고려해야만 된다.

대기압 플라즈마와 응용 (Atmospheric Plasma and Its Applications)

  • 엄환섭
    • 한국진공학회지
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    • 제15권2호
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    • pp.117-138
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    • 2006
  • 지표면에서 플라즈마는 전기방전에 의하여 만들어낸다. 그래서 대부분의 플라즈마 발생은 1백만분의 1기압보다 더 낮은 기압에서 발생하고 있었다. 그러나 많은 플라즈마 응용은 고기압에서 발생한 플라즈마를 요구하고 있다. 진공펌프와 같은 고가의 장비를 피하기 위하여 과학자들은 1기압이나 그이상의 압력에서 플라즈마를 발생하는 연구를 하기 시작했다. 많은 량의 제료 공정, 환경보호와 개선, 그리고 고효율 에너지 창출과 이용 등의 분야에 플라즈마를 사용할 때에는 오직 더 많은 량의 플라즈마를 더욱 값싸게 만들 때에만 가능한 것이다. 우리는 따라서 고기압에서 플라즈마를 만들어내는 새로운 방법을 개발하고 이러한 플라즈마가 21세기 산업에 적용될 수 있는 새로운 기반을 구축하는 연구를 수행하고 있다. 이러한 기술은 미래의 재료 공정이나, 환경 그리고 에너지 분야에 지대한 영향을 미칠 것으로 생각한다.

Numerical Simulation of the Characteristics of Electrons in Bar-plate DC Negative Corona Discharge Based on a Plasma Chemical Model

  • Liu, Kang-Lin;Liao, Rui-Jin;Zhao, Xue-Tong
    • Journal of Electrical Engineering and Technology
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    • 제10권4호
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    • pp.1804-1814
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    • 2015
  • In order to explore the characteristics of electrons in DC negative corona discharge, an improved plasma chemical model is presented for the simulation of bar-plate DC corona discharge in dry air. The model is based on plasma hydrodynamics and chemical models in which 12 species are considered. In addition, the photoionization and secondary electron emission effect are also incorporated within the model as well. Based on this model, electron mean energy distribution (EMED), electron density distribution (EDD), generation and dissipation rates of electron at 6 typical time points during a pulse are discussed emphatically. The obtained results show that, the maximum of electron mean energy (EME) appears in field ionization layer which moves towards the anode as time progresses, and its value decreases gradually. Within a pulse process, the electron density (ED) in cathode sheath almost keeps 0, and the maximum of ED appears in the outer layer of the cathode sheath. Among all reactions, R1 and R2 are regarded as the main process of electron proliferation, and R22 plays a dominant role in the dissipation process of electron. The obtained results will provide valuable insights to the physical mechanism of negative corona discharge in air.

플라즈마질화시 방전가스중 질소가스의 비율이 공구강(SKH51)의 질화층 및 미소경도에 미치는 영향 (Effects of Nitrogen Gas Ratio on Nitride Layer and Microhardness of Tool Steel(SKH51) in Plasma Nitriding)

  • 김덕재;이해룡;곽종구;정우창;조영래
    • 한국재료학회지
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    • 제12권6호
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    • pp.447-451
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    • 2002
  • Pulsed DC-plasma nitriding has been applied to form nitride layer having only a diffusion layer. The discharge current with the variation of discharge gases is proportional to the intensity of $N_2^+$ peak in optical emission spectroscopy during the plasma nitriding. The discharge current, microhardness in surface of substrate and depth of nitride layer increased with the ratio of $N_2\;to\;H_2$ gas in discharge gases. When the ratio of $N_2\;to\;H_2$ is lower than 60% in the discharge gases, high microhardness value of 1100Hv nitride layer which contains no compound layer has been formed.

대기압 Ar 가스의 직류 글로우 방전 특성분석 (Analysis on DC Glow Discharge Properties of Ar Gas at the Atmosphere Pressure)

  • 소순열
    • 전기학회논문지P
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    • 제59권4호
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    • pp.417-422
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    • 2010
  • Atmosphere Plasma of Gas Discharge (APGD) has been used in plasma sources for material processing such as etching, deposition, surface modification and so on due to having no thermal damages. The APGD researches on AC source with high frequency have been mainly processed. However, DC APGD studies have been not. In order to understand APGD further, it is necessary to study on fundamental properties of DC APGD. In this paper, we developed a one-dimensional fluid simulation model with capacitively coupled plasma chamber at the atmosphere pressure (760 [Torr]). Nine kinds of Ar discharge particles such as electron (e), positive ions ($Ar^+$, $Ar_2^+$) and neutral particles ($Ar_m^*$, $Ar_r^*$, $Ar_h^*$, $Ar_2^*$(1), $Ar_2^*$(3) and Ar gas) are considered in the computation. The simulation was worked at the current range of 1~15 [mA]. The characteristics of voltage-current were calculated and the structure of Joule heating were discussed. The spatial distributions of Ar DC APGD and the mechanism of power consumption were also investigated.

대향형 Xe 플라즈마 평판 램프의 방전 및 발광 특성에 관한 수치적 연구 (Numerical Analysis of the Discharge and Luminous Characteristics of a Planar Type Xe Plasma Flat Lamp)

  • 김혁환;이원종
    • 한국전기전자재료학회논문지
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    • 제24권10호
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    • pp.822-833
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    • 2011
  • A Xe plasma flat lamp, which has been noticed as a new eco-friendly LCD (liquid crystal display) backlight, requires the improvement of the luminance and the luminous efficiency although it has several advantages. To improve the performance of a lamp, it is necessary to understand the effects of discharge variables on the luminous characteristics of the lamp. Since it is difficult to diagnose a lamp discharge experimentally, the numerical analysis can be used instead. In this study, the luminous characteristics of a planar type Xe plasma flat lamp were analyzed with the variation of an input voltage and a pulse frequency. The numerical analysis of a lamp discharge was then performed using a RCT (relaxation continuum) model and a LFA (local field approximation) model. The comparison with the experimental results showed that the RCT model is valid for the numerical analysis of the flat lamp. The numerical analysis also showed that the modifications of a high frequency component and a voltage falling rate in the input voltage waveform could improve the luminous characteristics of the lamp.

Transport of space charge between sub-pixels in AC-plasma cell discharge

  • Lee, S.B.;Park, E.Y.;Han, Y.G.;Moon, M.W.;Oh, P.Y.;Song, K.B.;Lee, H.J.;Son, C.G.;Jeong, S.H.;Yoo, N.L.;Hong, Y.J.;Jeong, S.J.;Kim, J.H.;Park, S.O.;Choi, E.H.
    • 한국정보디스플레이학회:학술대회논문집
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    • 한국정보디스플레이학회 2006년도 6th International Meeting on Information Display
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    • pp.929-931
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    • 2006
  • In this experiment, we have investigated that the transported space charge between sub-pixels in AC-plasma cell discharge. The test pulse 30 V, $5{\mu}s$ was applied to the address electrodes of neighbor cells of discharge occurred cells. And we have measured the transported space charge between sub-pixels in accordance with the various last sustain pulse widths t(time gap between the rising edges of sustain and test pulses) of 0.2 to $3{\mu}s$. It was observed that the peak value of transported space charge has been shown to be 21.5pC at $1.0{\mu}s$. And the IR peak value have been occured after $0.51{\mu}s$ with respect to sustain voltage.

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