• 한국정밀공학회지
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• 제26권3호
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• pp.122-128
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• 2009

DBD(Dielectric Barrier Discharges) plasma is often used to clean the surface of semiconductor. The cleaning performance is affected mainly by plasma density and duration time. In this study, the plasma density is predicted by coupled simulation of flow, chemistry mixing and reaction, plasma, and electric field. 13.56 MHz of RF source is used to generate plasma. The effect of dielectric thickness, gap distance, and flow velocity on plasma density is investigated. It is shown that the plasma density increases as the dielectric thickness decreases and the gap distance increases.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2003년도 춘계학술대회
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• pp.1684-1689
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• 2003

Dielectric Barrier Discharges (DBD) in oxygen and air are well established for the production of large quantities of ozone and are more recently being applied to a wider range of after treatment processes for HAPs(Hazardous Air Pollutants). The potential use as a charger for particle collection are not well known. In this work, we measured charge distribution of nanometer or submicron sized particles passing through the dielectric barrier discharge reactor. The bipolar charge characteristics of particles passing DBD reactor were investigated. Fluorometric method using uranine particles and a fluorometer was employed to examine the bipolar charging characteristics of the charged particles by DBD reactor. Finally, the charge distributions of particles were determined from the electrical mobility classification using DMA.

• 대한전기학회논문지:전기물성ㆍ응용부문C
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• 제49권12호
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• pp.673-678
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• 2000

The dielectric barrier discharge(DBD) is a common method to create a nonthermal plasma in which electrical energy is used to create electrons with a high average kinetic energy. The unique aspect of dielectric barrier discharges is the large array of short lifetime(10ns) silent discharges created over the surface of the dielectric. A silent discharge is generated when the applied voltage exceeds the breakdown voltage of the carrier gas creating a conduction path between the applied electrode and grounded electrode. As charge accumulates on the dielectric, the electric field is reduced below the breakdown field of the carrier gas and the silent discharge self terminates preventing the DBD cell from producing a thermal arc. In fact, the most significant application of dielectric barrier discharges is to generate ozone for contaminated water treatment. Therefore, experiments were perfomed at 1∼2[bar] pressure using a coaxial geometry single dielectric barrier discharge for ozone concentrations and energy densities. The main result show that the concentration and efficiency of ozone are influenced by gas nature, gas quantity, gas pressure, supplied voltage and frequency.

• Applied Science and Convergence Technology
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• 제26권4호
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• pp.74-78
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• 2017

The discharge characteristics of the radio frequency (RF) surface dielectric barrier discharge have been simulated for the investigation of the ratio of the ion transit time to the RF period. From one-dimensional particle-in-cell (PIC) simulation for a planar dielectric barrier discharge (DBD), it was observed that the high-frequency driving voltage confines the ions in the plasma because of a shorter RF period than the ion transit time. For two-dimensional surface dielectric barrier discharges, a fluid simulation is performed to investigate the characteristics of RF discharges from 1 MHz to 40 MHz. The ratio of the peak density to the average density decreases with the increasing frequency, and the spatiotemporal discharge patterns change abruptly with the change in the ratio of ion transit time to the RF period.

• 전기학회논문지
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• 제61권5호
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• pp.717-720
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• 2012

Various types of dielectric-barrier-discharge (DBD) devices have been developed for diverse applications for the last decade. In this study, a flat non-thermal DBD micro plasma source under atmospheric pressure has been developed. The flat-panel type plasma is generated by bipolar pulse voltages, and driving gas is air. In this study, the plasma source was investigated with intensified charge coupled device (ICCD) images and Optical Emission Spectroscopy (OES). The micro discharges are generated on the crossed electrodes. For theoretical analysis, 2-dimensional fluid simulation was performed. The plasma source can be driven in air, and thus the operation cost is low and the range of application is wide.

• Korean Chemical Engineering Research
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• 제57권3호
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• pp.432-437
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• 2019

유연전극 기반의 대기압 부유전극 유전체 장벽 방전 (floating electrode-dielectric barrier discharge, FE-DBD) 시스템을 개발하여 플라즈마 특성을 분석하였다. 유연한 파워전극(powered electrode)을 구성하는 유연유전체로 polytetrafluoroethylene (PTFE), polydiemethylsiloxane (PDMS), polyethylene terephthalate (PET)를 사용하여 플라즈마를 발생하였을 때 플라즈마의 광학적 세기와 전자온도는 파워전극에 인가하는 전압이 증가할수록 증가하였고, 전압이 일정할 때는 PTFE < PDMS < PET 순으로 증가하였다. 이는 유전체의 종류와 전압에 따른 축전용량의 변화로 설명할 수 있었고, 유연전극 기반의 대기압 FE-DBD 플라즈마의 특성은 유연한 파워전극을 구성하는 유전체와 파워전극에 인가되는 전압을 변화함으로써 조절될 수 있음을 의미한다. 유연전극 대기압 FE-DBD 시스템은 피부 곡면을 따라 플라즈마가 발생될 수 있으므로 플라즈마 메디신(plasma medicine)에 유용할 것으로 기대한다.

• 한국융합학회논문지
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• 제13권3호
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• pp.281-289
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• 2022

플라즈마오존은 높은 살균성능으로 인해 다양한 살균분야에서 활용되고 있다. DBD(유전체 장벽방전)에 사용되는 유전체는 주로 석영, 세라믹, 폴리머 등이 주로 사용된다. 유전체로 이루어진 레이어는 공급되는 전하의 양을 제한시키고 플라즈마가 유전체 면 위에서 고르게 발생할 수 있도록 하는 역할을 한다. 이러한 DBD를 이용한 플라즈마, 오존살균은 살균대상이나 주변 환경이 복잡한 구조로 된 경우가 많아 공간살균에 대한 개념을 수립하고 이에 대한 연구와 학문적 체계가 필요하다. 본 연구에서는 플라즈마라디칼과 오존 생성을 위해 대기압에서 DBD방식을 이용한다. 플라즈마오존의 발생을 위한 반응기의 구조는 세라믹 튜브 유전체와 스테인리스 도체를 일정한 간격으로 배치하여 유전체 장벽방전을 발생시키는 형태이다. 공간살균장치로서의 플라즈마오존 발생은 성능 면에서 우수한 살균장치로 인식되고 있으므로 장치의 설계와 검증을 통해 공간살균장치의 최적설계를 확립하고자 하며 제안된 방법을 기반으로 다양한 살균 어플리케이션을 개발하는데 기초를 제공한다.

• Journal of Korean Society for Atmospheric Environment
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• 제18권E1호
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• pp.13-20
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• 2002

The electrical and chemical properties of the dielectric barrier discharge (DBD) process for the benzene removal were investigated. The benzene removal was initiated with the applied voltage higher than the discharge onset value. The removal efficiency over 95 % was obtained at approximately 1.6 kJ lite $r^{r-1}$ of the electrical energy density. The increase of the inlet concentration decreased the removal efficiency. However, the benzene decomposition rate increased with the inlet concentration . While the increase of the gas retention time enhanced the removal efficiency, the decomposition rate decreased. Identification of the optimum condition between the decomposition rate and the removal efficiency is required for field applications of the DBD process.s.

• 동굴
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• 제76호
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• pp.37-42
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• 2006

The Dielectric Barrier Discharge (DBD) is a nonequilibrium gas discharge that is generated in the space between two electrodes, which are separated by an insulating dielectric layer. The dielectric layer can be put on either of the two electrodes or be inserted in the space between two electrodes. If an AC or pulse high voltage is applied to the electrodes that is operated at applied frequency from 50Hz to several MHz and applied voltages from a few to a few tens of kilovolts rms, the breakdown can occur in working gas, resulting in large numbers of micro-discharges across the gap, the gas discharge is the so called DBD. Compared with most other means for nonequilibrium discharges, the main advantage of the DBD is that active species for chemical reaction can be produced at low temperature and atmospheric pressure without the vacuum set up, it also presents many unique physical and chemical process including light, heat, sound and electricity. This has led to a number of important applications such as ozone synthesizing, UV lamp house, CO2 lasers, et al. In recent years, due to its potential applications in plasma chemistry, semiconductor etching, pollution control, nanometer material and large area flat plasma display panels, DBD has received intensive attention from many researchers and is becoming a hot topic in the field of non-thermal plasma.

• 한국재료학회지
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• 제25권2호
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• pp.100-106
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• 2015

Plasma properties of dielectric barrier discharges (DBDs) at atmospheric pressure were measured and characterized using optical emission spectroscopy. Optical emissions were measured from argon, nitrogen, or air discharges generated at 5-9 kV using 20 kHz power supply. Emissions from nitrogen molecules were markedly measured, irrespective of discharge gases. The intensity of emission peaks was increased with applied voltage and electrode gap. The short wavelength peaks (315.9 nm and 337.1 nm) measured at the middle of DBDs were significantly increased with applied voltage. The optical emission from DBDs decreased with the addition of oxygen gas, which was especially significant in argon discharge. Emission from oxygen molecules cannot be measured from air discharge and argon discharge with 4.8% oxygen. The emission intensity at 337.1 nm and 357.7 nm related with nitrogen molecule was sensitively changed with electrode types and discharge voltages. However, the pattern of argon emission spectrum was nearly the same, irrespective of electrode type, oxygen content, and discharge voltage.