• Title/Summary/Keyword: Wall Voltage

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Wall Charge Distribution In the Address Period of AC Plasma Display Panel (AC PDP의 addressing 기간중의 벽전하 분포에 관한 연구)

  • Lee, Ki-Bum;Kim, Dong-Hyun;Kang, Dong-Sik;Park, Chung-Hoo;Cho, Chung-Soo
    • Proceedings of the KIEE Conference
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    • 2000.07c
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    • pp.1830-1833
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    • 2000
  • The relationships between driving voltage and the wall charge distribution in the address period of surface discharge type AC Plasma Display Panel have been investigated. The quantity of wall charge on each electrode are detected simultaneously from the electrode current after applying only one addressing discharge pulse. The wall charge Qy on the scan electrode Y is nearly the sum of Qx on the address electrode X and Qz on the sustain electrode 2. The Qy increased with the driving voltage regardless of the kind of electrode, whereas the address time Td decreased, Qz and Qy are increased considerably with the blocking voltage Vz, whereas Qx is decreased. The increase rate of Qx, Qy and Qz for increase in Vz was $-13{\times}10^{-2}$(pc/Vz), and $60{\times}10^{-2}$(pc/Vz) and $70{\times}10^{-2}$(pc/Vz), respectively.

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The Study on the Mutual Characteristics Between Transmitting Efficiency of Pulse Energy and Wall Plug Consumed Power of Non-Thermal Plasma (저온 플라즈마의 펄스에너지 전송효율과 Wall Plug 소비전력과의 상호 특성에 관한 연구)

  • Jeong, Jong-Han;Jeong, Hyeon-Ju;Kim, Hwi-Yeong;Jeong, Yong-Ho;Song, Geum-Yeong;Kim, Geun-Yong;Kim, Hui-Je
    • The Transactions of the Korean Institute of Electrical Engineers C
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    • v.51 no.10
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    • pp.506-510
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    • 2002
  • In this paper, we study on the mutual characteristics between transmitting efficiency of pulse energy and wall plug consumed power of non-thermal Plasma for removing environmental pollutive gas of coal plant. To obtain high pulse energy of our system, we used MPC(magnetic pulse compressor) of power switch and tested their characteristics by adjusting electrode length of reactor and charging voltage in capacitor. As a result, we obtained consumed power of wall plug and a compressed pulse of voltage 110kV, rising time 500ns. Impedance of load on increasing electrode length was decreased, but electrical efficiency was increased. These results indicate we can control critical voltage of pulse corona and electrical efficiency of economic cost in power plant.

Modified Driving Method for Reducing Address Time During Subfield Time in AC PDP (플라즈마 디스플레이 패널에서 부화면 시간동안 기입시간을 단축시키기 위한 수정된 구동파형)

  • Cho, Byung-Gwon
    • Journal of the Institute of Electronics and Information Engineers
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    • v.52 no.1
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    • pp.135-139
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    • 2015
  • The address discharge time lags are investigated in each subfield time in AC plasma display panel and a modified driving waveform is proposed to reduce the address discharge time lag by applying different additional scan voltage under no misfiring discharge production. The weak plasma discharge in AC PDP is generated by applying high positive-going ramp waveform to the scan electrode during the first reset period and that induce the production of the priming particle and wall charge. Because the wall charge becomes the wall voltage in a cell, the wall plus external address voltage produce the address discharge. However, as the wall charge in a cell is gradually disappeared as time passed, the address discharge time in the subfield time for 1 TV frame is lagged. In the first subfield time, the address discharge is faster produced than the other subfield time because the wall charge are much remained by the high positive-going ramp voltage during the reset period in the first subfield time. Meanwhile, from the second to last subfield, the address discharge production time is gradually delayed due to the dissipation of the wall charge in a cell. In this study, the address discharge time lags are measured in each subfield time and the total address discharge time lags are shortened by applying the different additional scan voltage during the address period in each the subfield time.

Wall charge & Wall Voltage Characteristics on Sustain Driving Voltage in AC PDP

  • 김태영
    • Proceedings of the Korean Vacuum Society Conference
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    • 1999.07a
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    • pp.237-237
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    • 1999
  • 전극폭 300um, 전극간격 100um, 격벽높이 130um로 자체 제작한 테스트 패널에서 방전개시전압과 최소 방전유지전압 사이에서 방전유지전압 변화에 따른 벽전하, 벽전압을 측정하였다. 이 실험에서는 Ne가스와 Ne-Xe 혼합가스를 이용하였다. 이 결과로부터 방전유지전압 변화에 따른 벽전하, 벽전압을 통하여 최적의 방전유지전압 조건을 결정할 수 있으며, 이는 AC-PDP의 효율 향상에 기여할 것으로 판단되어 진다.

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The effects of discharge gases in the voltage transfer curve of ac-PDP (ac-PDP의 전압전달특성에 미치는 방전가스의 영향)

  • Son, J.B.;Lee, S.H.;Kim, D.H.;Kim, Y.D.;Cho, J.S.;Park, J.H.
    • Proceedings of the KIEE Conference
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    • 1999.07e
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    • pp.2233-2235
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    • 1999
  • The ac plasma display panel(PDP) is a flat light-emitting gas discharge device. Discharge gases directly take effects to the discharge phenomena of ac PDP. Therefore it is necessary to understand the characteristics of the discharge gases. In this paper, we have studied the effects of discharge gases by voltage transfer curves which show the discharge characteristics of ac PDP and the change of the effective wall capacitance during a discharge which depends on lateral spreading of charge distribution and the strength of discharge. As gas pressure increases, memory margins increases. and the firing voltage of a mixed gas is lower than that of a single gas such as He gas. The minimum sustain voltage and the maximum sustain voltage or firing voltage increases with decrease in the frequency. The effective wall capacitance increases as the discharge strength that is, the gap voltage between discharge electrodes increases.

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Characteristics of Particle Deposition onto the Cleanroom Wall Panel with Electrostatic Voltages (정전압에 따른 클린룸 벽체에서의 입자침착 특성)

  • Noh, Kwang-Chul;Son, Young-Tae;Kim, Jong-Jun;Oh, Myung-Do
    • Korean Journal of Air-Conditioning and Refrigeration Engineering
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    • v.18 no.12
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    • pp.1033-1038
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    • 2006
  • We carried out the experiments on particle deposition onto the cleanroom wall panels. And then we investigated the particle deposition characteristic coefficients for electrostatic voltages and particle size. It was found that there is little difference in characteristics of the particle deposition between the steel panel and the anti-static coating panel. In case of that the particle size is under $1.0{\mu}m$, the particle deposition characteristic coefficient becomes larger as the electrostatic voltage induced to the cleanroom wall panel is increasing. Where in case of that the particle size is over $3.0{\mu}m$, the particle deposition characteristic coefficients do not show any differences with the electrostatic voltages. It is due to that the electrostatic force is the major particle transport mechanism for submicron particles, while the gravitational settling is the major particle transport mechanism for overmicron particles when the electro-static voltages are induced to the cleanroom wall panel.

Wall Charge Measurement in the Address Period of AC Plasma Display Panel

  • Kim, Dong-Hyun;Lee, Sung-Hyun;Kim, Young-Dae;Park, Jung-Tae;Lee, Gi-Bum;Lee, Jae-Young;Ryu, Jae-Hwa;Park, Chung-Hoo
    • Journal of Information Display
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    • v.1 no.1
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    • pp.42-47
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    • 2000
  • The relationship between driving voltage and the amount of wall charge in the address period of surface discharge type AC Plasma Display Panel has been investigated. The amount of wall charge on each electrode is obtained simultaneously from the current profiles after applying only one addressing discharge pulse. The wall charge $Q_y$ on the scan electrode Y is almost the sum of $Q_x$ on the address electrode X and $Q_z$ on the sustain electrode Z. The $Q_y$ increased with the driving voltage regardless of the kind of electrode, whereas the addressing $T_d$ decreased. The $Q_x$ and $Q_y$ are increased considerably by blocking voltage $V_z$, whereas $Q_x$ is decreased. The $V_z$ dependence of $Q_x$ $Q_y$ and ${\varrho}_z$ in addressing discharge was $-13{\times}10^{-2}$ (pc/$V_z$), and $60{\times}10^{-2}$ ($pc/V_z$) and $70{\times}10^{-2}(pc/V_z)$, respectively.

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Electric Properties of Mercury-free Xe EEFL (무수은 제논 EEFL의 전기적 특성)

  • Lee, Seong-Jin;Kim, Nam-Goon;Lee, Jong-Chan;Park, Noh-Joon;Park, Dae-Hee
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.20 no.7
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    • pp.650-657
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    • 2007
  • This paper had mentioned about CCP light source application for increasing the efficiency of Xe lamp the mercury-free lamp. In order to increase the efficiency of Xe EEFL, we designed and manufactured the lamp used by mixture gas of Xe, Ne and He. Also, we have analyzed the electrical and optical properties with the firing voltage, sustain voltage, paschen's curve, wall charge, and capacitance. As a result, the firing voltage decreased by increasing the ration of mixture gas. and, It is owing to include the gas with high ionization energy. The firing voltage decreased in condition happening the penning effect, Because the ion of metastable state created from penning effect, Which can encourage the ionization phenomena. Also, the wavelength of 467.12 is increase. because of the energy transition in the wavelength of 147 nm. therefore, we can know about the affection of phosphor with UV emission properties. Through an experiment, Xe 100 % and Xe 75 % confirmed same spectrum properties by each mixture gas ratio. In the case of Xe 50 %, spectrum properties appeared Xe discharge and Ne-He discharge. That analyzed an electrical and optical properties. Therefore, confirmed that is excellent because properties of firing voltage, wall charge, capacitance in Xe 50 %, Ne : He = 9 : 1. We offered parameter in inverter manufacture and lamp manufacture by electrical and optical properties.

A Comparative Study on Discharge Characteristics of FHD and QFHD AC PDP (FHD와 QFHD 해상도를 가지는 AC PDP의 방전특성 비교연구)

  • Choi, Yong-Suk;Heo, Jun;Kim, Dong-Hyun;Lee, Hae-June;Lee, Ho-Jun
    • The Transactions of The Korean Institute of Electrical Engineers
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    • v.60 no.1
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    • pp.119-123
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    • 2011
  • We have investigated the luminous efficiency of various cell resolution and structure from 50" FHD to 50" QFHD Plasma Display. The suggested test panels have two different cell array types which are the delta and matrix cell array type. The results showed that, in the case of the suggested QFHDs, the firing and sustain voltage were increased and voltage margin was decreased. These results are caused by the reduced wall voltage and increased charged particle loss, at the side wall. The luminance of the suggested QFHDs was lower from 20% to 40% than that of the suggested FHDs and the power consumption was higher from 42% to 83% than that of the suggested FHDs. In conclusion, the maximum luminous efficiency of the suggested QFHD(D110) has reached about 38%, compared with suggested FHDs($\fallingdotseq$ 2.7 lm/W).