• 한국광학회지
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• 제12권2호
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• pp.115-120
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• 2001

본 연구는 고온 고압의 전열(electrothermal)플라즈마내에 존재하는 구리원자의 발광 스펙트럼을 정량적으로 분석하는 방법에 대해 논하였다. 플라즈마는 플라즈마 발생장치내에 설치되어 있는 모세관 양단의 두 개의 전극이 방전함으로써 발생하며 고속으로 대기를 향해 전파해 나간다. 플라즈마의 특성을 분석하기 위해서는 플라즈마의 여기온도나 전자밀도와 같은 물리량의 측정이 필요하다. 그러나 여기온도나 전자밀동와 직접적으로 관련이 있는 발광 스펙트럼은 분광시스템의 파장에 따른 서로다른 응답 특성 때문에 왜곡되어질 수 있다 따라서 본 연구에서는 펄스 플라즈마 제트로부터 얻은 구리원자의 발광 스펙트럼을 정밀하게 보정하는 방법을 제시하였다.

• 한국항공우주학회지
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• 제32권8호
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• pp.47-53
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• 2004

타원형 날개꼴의 공력 특성에 브로잉 제트 방식과 제트 방향의 영향에 대하여 실험을 통하여 연구를 수행하였다. 본 연구는 타원형 날개꼴의 박리제어에 있어서 브로잉 제트적용에 관한 기본 데이터를 축적하는데 목적을 두었다. 본 연구에서는 날개면에서의 압력 분포, 브로잉 제트 출구에서의 유속 분포 및 공력 자료를 제공하였다. 타원형 날개꼴에 대한 실험은 레이놀즈수 $8.22{\times}10^5$에서 수행하였다. 펄스제트는 후실속각 이후에 공력 특성을 향상시키는 효과를 보여 주었다. 즉, 펄스제트는 감소된 질량유동율로 상당히 높은 양력을 발생하였다. 제트 방향도 박리제어의 주요 파라미터임을 보였다. 양의 제트각은 박리를 지연시키거나 억제하였고, 음의 제트각은 박리를 오히려 촉진시켰다.

• 한국가시화정보학회:학술대회논문집
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• 한국가시화정보학회 2002년도 추계학술대회 논문집
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• pp.43-44
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• 2002

A pulsed jet was measured with high-definition 3D-PTV technique. The measurement system consists of three CCD cameras, Ar-ion laser, an image grabber and a host computer. Two fitness functions were introduced in a genetic algorithm in order to enhance the correspondences of the particles. One was based on a concept of the continuum theory and the other one was based on a minimum distance error. The head vortex of the jet was visualized by LIF and was reconstructed by the constructed high-resolution 30-PTV system for comparisons.

• Journal of Mechanical Science and Technology
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• 제15권12호
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• pp.1808-1815
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• 2001

The characteristics of a pulsed plasma jet originating from an electrothermal capillary discharge have been investigate using laser-induced fluorescence (LIF) measurement. Previous emission measurements of a 3.1 kJ plasma jet show trial upstream of the Mach disk the temperature and electron number density are about 14,000 K and and 10$\^$17/ cm$\^$-3/, while downstream of the Mach dick tole values are about 25,000 K and 10$\^$18/ cm$\^$-3/, respectively. However, these values are barred on line-of-sight integrated measurements that may be misleading. Hence, LIF is being used to provide both spatially and temporally resolved measurements. Our recent work has been directed at using planar laser-induced fluorescence (PLIF) imaging of atomic copper in the plasma jet flow field. Copper is a good candidate for PLIF studies because it is present throughout the plasma and has electronic transitions that provide an excellent pump-detect strategy. Our PLIF results to date show that emission measurements may give a misleading picture of the flow field, as there appeals to be a large amount of relatively low temperature copper outside the barrel shock. which may lead to errors in temperature inferred from emission spectroscopy. In this paper, the copper LIF image is presented and at the moment, relative density of atomic copper, which is distributed in the upstream of the pulsed plasma jet, is discussed qualitatively.

• 한국항공우주학회지
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• 제45권11호
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• pp.907-913
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• 2017

아크 플라즈마에 의해 구동되는 스파크 제트의 다양한 에너지 공급 방법에 따른 효율적 운전 성능 특성에 대한 실험적 연구를 수행하였다. 펄스 당 37 mJ의 주입 에너지에 의한 급속한 기체의 가열에 의해 약 330 m/s의 고속 제트가 발생함을 확인하였다. 제트의 최대 속도와 침투 거리는 각각 주입된 전력량과 펄스 당 주입된 에너지에 비례하였다. 낮은 에너지에서는 오리피스 직경이 작을수록 더 높은 속도의 제트가 발생하였다. 공급 에너지가 같다면 전류를 높인 펄스가 펄스 폭을 높인 펄스보다 높은 속도의 제트를 발생시켰다. 펄스 폭이 약 $10{\mu}s$이고 펄스 당 에너지가 약 10 mJ인 경우가 효율적인 운전에 보다 더 적합한 것으로 확인되었다.

• 한국전산유체공학회:학술대회논문집
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• 한국전산유체공학회 2008년도 춘계학술대회논문집
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• pp.593-596
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• 2008

Because of good performance of heat transfer characteristics, impinging jets are widely used in many industries for cooling or heating. And the present num erical studies attempt to show the effects of impinging jet. This paper considers the application of the turbulent models to impinging jet flow with pulsed inlet. It is assumed two-dimensional turbulent flows. The jet Reynolds num ber is set at 23,000 and the distance from the exit of the nozzle to the plate is 3 times larger than the diam eter of the nozzle. The influence of the Strouhal num ber(pulsation frequency) on Nusselt number at the impinging region is investigated. Strouhal numbers are ranged 0.0 to 0.5 and the forcing amplitudes are 1%,5%,9% of mean inlet velocity. In this study, the Nusselt number at the impinging region is sensitive to the pulsation frequency. Heat transfer coefficient strongly increase at Strouhal num ber of 0.4.

• Journal of Advanced Marine Engineering and Technology
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• 제28권8호
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• pp.1211-1224
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• 2004

Two round jets. impinged and pulsed. were measured with high-resolution 3D-PTV technique. The measurement system consists of three CCD cameras, Ar-ion laser, an image grabber and a host computer. Two fitness functions were introduced in a genetic algorithm in order to enhance the correspondences of the particles. One was based on a concept of the continuum theory and the other one was based on a minimum distance error. The velocity profiles of the impinged jet obtained by the constructed 3D-PTV system were compared with those of LDV measurements made in this study. The head vortex of the jet was visualized by LIF and was reconstructed by the constructed high-resolution 3D-PTV system for comparisons.

• 한국전산유체공학회:학술대회논문집
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• 한국전산유체공학회 2008년도 춘계학술대회논문집
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• pp.61-64
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• 2008

The present study of these experiments are close examination of spray characteristics that are continuous liquid jet and modulated pressure pulse liquid jet. The experiments were conducted using water, over a range of cross-flow velocities from 42${\sim}$136 m/s, with injection frequencies of 35.7${\sim}$166.2 Hz. Between continuous cross-flow jet and pressure pulsed cross-flow jet for characteristics of penetration, breakup point, spray angle and macro spray shape are investigated experimentally. In cross-flow field, main parameter of liquid jet for breakup was cross-flow stream rather than pressure pulse frequency. As oscillation of the periodic pressure that could make liquid jet moved up and down, the mixing efficiency was increased. Also, a bulk of liquid jet puff was detected at upper field of liquid surface. So, this phenomenon has a good advantage of mixing spray from concentration of center area to outer area. Because of pressure pulsation frequency, an inclination of SMD for the structured layer was evanescent. Cross-sectional characteristics of SMD at downstream area were non-structured distributions. Then cross-sectional characteristics of SMD size were about same tendency over a range that is effect of spray mixing. The tendency of volume flux value for various frequency of pressure pulse was same distribution. And volume flux was decreased when the frequency of pressure pulse increase.

• Journal of Microbiology and Biotechnology
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• 제25권3호
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• pp.381-385
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• 2015

In the present study, drop-on-demand two-dimensional patterning of unstained and stained bacterial cells on untreated clean wafers was newly conducted using an electrospray pulsed jet. We produced various spotted patterns of the cells on a silicon wafer by varying the experimental conditions, such as the frequency, flow rate, and translational speed of the electrospray system in a two-dimensional manner. Specifically, the electrospray's pulsed jet of cell solutions produced alphabetical patterns consisting of spots with a diameter of approximately $10{\mu}m$, each of which contained a single or a small number of viable bacteria. We tested the viability of the patterned cells using two visualization methods. This pattering technique is newly tested here and it has the potential to be applied in a variety of cell biology experiments.

• 한국마린엔지니어링학회:학술대회논문집
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• 한국마린엔지니어링학회 2006년도 전기학술대회논문집
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• pp.53-54
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• 2006

Experimental analyses on the Hydroelastic Flow-Structure Interactions on pulsed impinged jet is measured with the FSIMS(Flow-Structure Interaction Measurement System. The nozzle diameter is D=15mm and two major experiments have been carried out for the cases of the distance between the nozzle tip to the elastic wall is 6.0. The pulsed jets were controlled by a solenoid valve and were impinged onto an elastic plate (material: silicon, diameter: 350mm, thickness: 0.5mm, hardness: 15). The Reynolds numbers were 20,000 and 24,000 when the jets were impinged with the volume velocities. The results showed that the elastic plate moved slightly to the opposite direction of the jet direction at the time of valve opening. It has been shown that the vortices travelling over the surface of the wall made the elastic wall distorted locally due to a vector forces between rotating forces of the vortex and a newly-incoming flow.