• Title/Summary/Keyword: Sheet Beam

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An Experimental Study on the Injector-spray Behavior of a Liquid-propellant Thruster (액체추진제 추력기의 인젝터 분무 거동에 대한 실험적 연구)

  • Kim, Jin-Seok;Kim, Sung-Cho;Park, Jeong;Kim, Jeong-Soo
    • Journal of the Korean Society for Aeronautical & Space Sciences
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    • v.35 no.9
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    • pp.799-804
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    • 2007
  • The behavior of spray emanating from an injector to be employed in a liquid-propellant thrust chamber is investigated by optical measurement techniques. The injector has eight holes, each of which has 30 cant angle from the center-axis with the diameter of 0.406 mm. In order to examine an atomization process according to the spray-generation conditions and the evolution along spray downstream, variational features in the velocity and size of droplets obtained through Dual-mode Phase Doppler An 799emometry (DPDA) are delineated and discussed together with instantaneous plane images captured by using Nd:Yag laser sheet beam. A categorization of spray-flow regime representing the atomization and turbulent nature is made through evaluating the non-dimensional parameters, i.e., Reynolds number and Weber number based upon the theoretical injection velocity. These qualitative and quantitative data of spray breakup will be a firm basis for the design of brand-new thruster

Visualization Study of High-Incidence Vortical Flow over the LEX/Delta Wing Configuration with Sideslip (옆미끄럼을 갖는 LEX/삼각 날개 형상에 대한 높은 받음각 와유동의 가시화 연구)

  • Sohn, Myong-Hwan;Lee, Ki-Young
    • Journal of the Korean Society for Aeronautical & Space Sciences
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    • v.30 no.5
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    • pp.109-117
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    • 2002
  • An off-surface flow visualization experiments have been performed to investigate the flow field over a delta wing with the leading edge extension(LEX). The model is a flat wing with $65^{\circ}$ sweepback angle. The free stream velocity is 6.2 m/s, which corresponds to Reynolds number of $4.4\times10^5$ based on the wing root chord. The angle of attack and sideslip angle range from $16^{\circ}\sim28^{\circ}$ and $0^{\circ}\sim-15^{\circ}$, respectively. The visualization technique of using the micro water-droplet and the laser beam sheet enabled to observe the vortical flow structures, which can not be obtained by 5-hole probe measurements. With sideslip angle, the interaction and breakdown of the LEX and wing vortices was promoted in the windward side, whereas, it was suppressed in the leeward side.

Growth of 2dimensional Hole Gas (2DHG) with GaSb Channel Using III-V Materials on InP Substrate

  • Sin, Sang-Hun;Song, Jin-Dong;Han, Seok-Hui;Kim, Tae-Geun
    • Proceedings of the Korean Vacuum Society Conference
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    • 2011.02a
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    • pp.152-152
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    • 2011
  • Silicon 기반의 환경에서 연구 및 제조되는 전자소자는 반도체의 기술이 발전함에 따라 chip 선폭의 크기가 30 nm에서 20 nm, 그리고 그 이하의 크기로 점점 더 작아지는 요구에 직면하고 있다. 탄소나노 구조와 나노와이어 기술이 Silicon을 대신할 다음세대 기술로 주목받고 있다. 많은 연구결과들 중에서 III-V CMOS가 가장 빠른 접근 방법이라 예상한다. III-V족 물질을 이용하면 electron 보다 수십 배 이상의 이동도를 얻을 수 있으나 p-type의 구조를 구현하는 것이 해결해야 할 문제이다. p-type 3-5 족 화합물을 이용하여 에너지 밴드 갭의 변화를 가능하게 한다면 hole의 이동도를 크게 향상시킬 수 있어 silicon 기반의 p-type 소자보다 2~3배 더 빠른 소자의 구현이 가능하다. 3-5족 화합물 반도체의 성장 기술이 많이 진보되어 이를 이용하여 고속 소자를 구현한다면 시기적으로 더욱 빨리 다가올 것이라 예측한다. 에너지 밴드갭의 변화와 격자 부정합을 고려하여 SI InP 기판에 GaSb 물질을 채널로 사용한 p-type 2-dimensional hole gas (2DHG) 소자를 구현하였다. 관찰된 소자 구조의 박막 상태의 특징을 보이며 10 um ${\times}$ 10 um AFM 측정결과 1 nm 이하의 표면 거칠기를 가지며 상온에서의 hole 이동도는 약 650 cm2/Vs이고 sheet carrier density는 $5{\times}1012$ /cm2의 결과를 확인하였다. 실험결과 InP 기판위에 채널로 사용된 GaSb 박막을 올리는데 있어 가장 중요한 것은 Phosphorus, Arsenic, 그리고 Antimony 물질의 양과 이들의 변화시간의 조절이다. 본 발표에서 Semi-insulating InP 기판위에 electron이 아닌 hole을 반송자로 이용한 차세대 고속 전자소자를 구현하고자 하여 MBE (Molecular Beam Epitaxy)로 p-type 소자를 구현하여 실험하였다. 아울러 더욱 빠른 소자의 구현을 위하여 세계의 유수 그룹들의 연구 결과들과 앞으로 예상되는 고속 소자에 대해서 비교와 함께 많은 기술에 대해 논의하고자 한다.

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Visualization and Flowfield Measurements of the Vortical Flow over a Double-Delta Wing

  • Sohn, Myong-Hwan;Jang, Young-IL
    • International Journal of Aeronautical and Space Sciences
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    • v.4 no.1
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    • pp.63-74
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    • 2003
  • The vortical flow of a 65-deg flat plate delta wing with a leading edge extension(LEX) was examined through off-surface visualization, 5-hole probe and hot-film measurements. The off-surface flow visualization technique used micro water droplets generated by a home-style ultrasonic humidifier and a laser beam sheet. The angles of attack ranged from 10 to 30 degrees, and the sideslip angles ranged from 0 to -15 degrees. The Reynolds number was $1.82{\times}10^5$ for the flow visualization, and $1.76{\times}10^6$ for the 5-hole probe and hot-film measurements. The comparison of the visualization photos and the flow field measurement showed that the two results were in a good agreement for the relative position and the structure of the wing and LEX vortices, even though the flow Reynolds numbers of the two results were much different. The wing vortex and the LEX vortex coil each other while maintaining a comparable strength and identity at zero sideslip. Neither a looping of the wing vortex around the strake vortex, nor the lopsided coiling of the stronger strake and the weaker wing vortices was observed. At non-zero sideslip, the downward movement of the LEX vortex when going downstream was enhanced on the windward side, and the downward and inboard movement of the LEX vortex when going downstream was suppressed on the leeward side. The counterclockwise coiling of the wing and LEX vortices was decreased significantly on the leeward side.

Junction Area Dependence of Tunneling Magnetoresistance in Spin-dependent Tunneling Junction with Natural $Al_2O_3$Barrier (자연산화 $Al_2O_3$장벽층을 갖는 스핀의존 터널링 접합에서 자기저항특성의 접합면적 의존성)

  • 이긍원;이상석
    • Journal of the Korean Magnetics Society
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    • v.11 no.5
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    • pp.202-210
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    • 2001
  • Spin dependent tunneling (SDT) junction devices of Ta/NiFe/Ta/NiFe/FeMn/NiFe/AlOx/CoFe/NiFe/Al with in-situ naturally oxidized Al barrier were fabricated using ion beam deposition and dc sputtering in UHV chamber of 10$^{-9}$ Torr. The maximum tunneling magnetoresistance (TMR) and the product resistance by junction (R$_{j}$ A) are 16-17% and 50-60 $\Omega$${\mu}{\textrm}{m}$$^2$, respectively. The values of TMR and (R$_{j}$ A) with field annealing were slightly increased. The TMR and (R$_{j}$ A) dependence versus the junction area size was observed. These results were explained by using sheet resistance effect of bottom electrode and spin channel effects.

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Summer Marine Algal Floras and Community Structures in Taean Peninsula, Korea (태안반도 하계 해조상 및 군집구조)

  • Yoo, Hyun-Il;Lee, Ji-Hee;Lee, Ki-Hun;Baek, Sang-Hum;Heo, Young-Beam;Noh, Hyoung-Soo;Choi, Han-Gil
    • Korean Journal of Fisheries and Aquatic Sciences
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    • v.40 no.4
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    • pp.210-219
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    • 2007
  • The benthic marine algal flora and community structure were examined at five sites of the Taean Peninsula, Korea, during July-August 2005. Ninety-six algal species were Identified, including 14 green, 21 brown, and 60 red algae, and 1 marine plant. The common species that occurred at the five sites were Sargassum thunbergii, Gelidium divaricatum, Caulacanthus okamurae, Gracilavia vermiculophylla, and Neorhodomela aculeata. Sthunbergii was the dominant species in terms of coverage and biomass at ail of the study sites. The average biomass varied from $23.72g/m^2$ in dry weight at Chaeseokpo to $66.43g/m^2$ at Padori. The species could be divided into six functional groups in terms of morphological characteristics: 41 coarsely branched forms, 25 filamentous forms, 16 sheet forms, 7 thick leathery forms, including the marine plant Phyllospadix iwatensis, 4 crustose forms, and 3 Jointed calcareous forms. The seaweed communities at the five study sites were unstable and the environmental conditions were bad or very bad. Among the five study sites, the ecological evaluation index (EEI) and diversity index (H') were maximal at Padori at 2.29 and 1.98, respectively. By contrast, the dominance index (DI) was minimal at Padori (0.55) and maximal at Baramarae (0.96). Therefore, we conclude that the rocky shore at Padori has the best environment among the five study sites, although the species richness and biomass of seaweeds have declined continuously over the last 10 years.

Control of Explosion Behavior in Micro Hole Using UV Laser on LTCC Green Sheets Containing Carbon Particles (카본을 첨가한 LTCC 그린 시트에서 UV 레이저를 이용한 미세 홀 터짐 현상 제어)

  • Kim, Shi Yeon;Ahn, Ik-Joon;Yeo, Dong-Hun;Shin, Hyo-Soon;Yoon, Ho Gyu
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.29 no.12
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    • pp.786-790
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    • 2016
  • Hole explosion behaviors were observed during drilling fine holes with laser beam on the LTCC green bar of $320{\mu}m$ thick after lamination of green sheets prepared by tape casting of thick film process. The incidence of these hole explosions was inversely proportional to hole sizes. The incidence of hole explosion was 20 % number of hole with the size of $60{\mu}m$ exploded for the UV radiation, while the explosion did not appear for hole sizes over $100{\mu}m$. To prevent hole explosion behavior during laser-drilling of fine holes, carbon black powder was added as an additive in the LTCC composition, which has superior thermal durability. As a consequence, hole explosion rate was suppressed to 0.8 % for the hole size of $50{\mu}m$ green sheet with the carbon black amount of 10 weight % and the laser power of 3 watt. Added carbon is thought to reduce the heat-affected region during laser drilling.

Study on the deposition rate and vapor distribution of Al films prepared by vacuum evaporation and arc-induced ion plating (증착방법에 따른 Al 피막의 증착율 및 증기분포에 관한 연구)

  • 정재인;정우철;손영호;이득진;박성렬
    • Journal of the Korean Vacuum Society
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    • v.9 no.3
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    • pp.207-215
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    • 2000
  • Al films on cold-rolled steel sheet have been prepared by vacuum evaporation and arc-induced ion plating, respectively, and the evaporation rate and vapor distribution (thickness distribution over the substrate) have been investigated according to deposition conditions. The arc-induced ion plating (AIIP) method have been employed, which makes use of arc-like discharge current induced by ionization electrode located near the evaporation source. The AIIP takes advantage of high ionization rate compared with conventional ion plating, and can be carried out at low pressure of less than $10^{-4}$ torr. Very high evaporation rate of more than 2.0 mu\textrm{m}$/min could be achieved for Al evaporation using alumina liner by electron beam evaporation. The geometry factor n for the $cos^{n/\phi}$ vapor distribution, which affects the thickness distribution of films at the substrate turned out to be around 1 for vacuum evaporation, while it features around 2 or higher for ion plating. For the ion plated films, it has been found that the ionization condition and substrate bias are the main parameters to affect the thickness distribution of the films.

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The Effect of Tool Geometry on the Mechanical Properties in a Friction Stir Welded Lap Joint between an Al Alloy and Zn-coated Steel (알루미늄 합금과 아연도금강판의 이종 겹치기 마찰교반접합에서 기계적성질에 미치는 Tool Geometry의 영향)

  • Kim, Nam-Kyu;Kim, Byung-Chul;Jung, Byung-Hoon;Song, Sang-Woo;Nakata, K.;Kang, Chung-Yun
    • Korean Journal of Metals and Materials
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    • v.48 no.6
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    • pp.533-542
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    • 2010
  • The specific motivation for joining an Al alloy and Zn-coated steel arises from the need to save fuel consumption by weight reduction and to enhance the durability of vehicle structures in the automobile industry. In this study, the lap joining A6K31 Al alloy (top) and SGARC340 Zn-coated steel (bottom) sheets with a thickness of 1.0 mm and 0.8 mm, respectively, was carried out using the friction stir weld (FSW) technique. The probe of a tool did not contact the surface of the lower Zn-coated steel sheet. The friction stir welding was carried out at rotation speeds of 1500 rpm and travel speeds of 80~200 mm/min. The effects of tool geometry and welding speed on the mechanical properties and the structure of a joint were investigated. The tensile properties for the joints welded with a larger tool were better than those for the joints done with a smaller tool. A good correlation between the tensile load and area of the welded region were observed. The bond strength using a larger tool (M4 and M3) decreased with an increase in welding speed. Most fractures occurred along the interface between the Zn-coated steel and the Al alloy. However, in certain conditions with a lower welding speed, fractures occurred at the A6K31 Al alloy.

Property of Nickel Silicide with 60 nm and 20 nm Hydrogenated Amorphous Silicon Prepared by Low Temperature Process (60 nm 와 20 nm 두께의 수소화된 비정질 실리콘에 따른 저온 니켈실리사이드의 물성 변화)

  • Kim, Joung-Ryul;Park, Jong-Sung;Choi, Young-Youn;Song, Oh-Sung
    • Journal of the Korean Vacuum Society
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    • v.17 no.6
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    • pp.528-537
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    • 2008
  • 60 nm and 20 nm thick hydrogenated amorphous silicon(a-Si:H) layers were deposited on 200 nm $SiO_2$/single-Si substrates by inductively coupled plasma chemical vapor deposition(ICP-CVD). Subsequently, 30 nm-Ni layers were deposited by an e-beam evaporator. Finally, 30 nm-Ni/(60 nm and 20 nm) a-Si:H/200 nm-$SiO_2$/single-Si structures were prepared. The prepared samples were annealed by rapid thermal annealing(RTA) from $200^{\circ}C$ to $500^{\circ}C$ in $50^{\circ}C$ increments for 40 sec. A four-point tester, high resolution X-ray diffraction(HRXRD), field emission scanning electron microscopy(FE-SEM), transmission electron microscopy(TEM), and scanning probe microscopy(SPM) were used to examine the sheet resistance, phase transformation, in-plane microstructure, cross-sectional microstructure, and surface roughness, respectively. The nickel silicide from the 60 nm a-Si:H substrate showed low sheet resistance from $400^{\circ}C$ which is compatible for low temperature processing. The nickel silicide from 20 nm a-Si:H substrate showed low resistance from $300^{\circ}C$. Through HRXRD analysis, the phase transformation occurred with silicidation temperature without a-Si:H layer thickness dependence. With the result of FE-SEM and TEM, the nickel silicides from 60 nm a-Si:H substrate showed the microstructure of 60 nm-thick silicide layers with the residual silicon regime, while the ones from 20 nm a-Si:H formed 20 nm-thick uniform silicide layers. In case of SPM, the RMS value of nickel silicide layers increased as the silicidation temperature increased. Especially, the nickel silicide from 20 nm a-Si:H substrate showed the lowest RMS value of 0.75 at $300^{\circ}C$.