• 콘크리트학회논문집
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• 제26권6호
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• pp.707-714
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• 2014

콘크리트 충전강관(CFT)은 강관의 내부에 콘크리트로 채워진 기둥이다. CFT는 강재와 콘크리트로 구성되며, 강재는 콘크리트를 내부에서 구속시켰고, 내부 콘크리트는 기둥의 압축하중을 감당한다. 본 실험에서 73~100MPa급 고강도 콘크리트에 관해 유동성실험, 압축강도실험, 압송압력실험을 실시하였으며, CFT용 고강도 콘크리트의 물리적 성질을 알아보기 위해 슬럼프, 슬럼프 플로우, 공기량, U-box시험, O-Lot시험, L-flow시험이 진행되었다. 이러한 연구의 결과를 바탕으로 Mock-up테스트에서 콘크리트 충전성 시험, 수화열 측정 시험, 응력계측 시험을 수행하였다. 현장적용은 상암동 및 서강대 현장의 두 곳에 각각 ${\Box}-566{\times}566{\times}10$, ${\Box}-400{\times}400{\times}25$의 대상기둥을 선정하여 현장계측을 진행하였다. CFT기둥의 장기거동 예측에 관하여 설계하중에 대해 콘크리트의 탄성변형과 건조수축, 크리프 수축을 고려한 ACI 209 재료모델을 사용한 결과는 계측결과와 거의 일치하였다.

• 센서학회지
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• 제6권3호
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• pp.172-179
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• 1997

간섭형 광섬유 센서의 경우 소자의 구성만 적절히 바꾸어 다른 종류의 측정에도 사용될 수 있다는 점에 착안하여 여러 종류의 센서를 동시에 신호처리할 수 있는 원격 다중화 광섬유 센서 시스템을 구현하였다. 구현된 센서 시스템의 신호처리는 간단한 광학 구성으로 원격 다중화 측정이 가능하도록 광섬유 Fabry-Perot 간섭형 센서배열을 가정하여 피측정량의 변화에 의한 간섭 무늬의 수만 카운트하는 디지털 신호처리로 구성되었다. 광섬유의 광학 효과에 대한 데이터를 종합함으로써 센서 시스템에 부착할 센서를 구현하기 위해 적합한 광학효과를 선택하는 기준을 제시하였으며, 한 예로서 반경 4.3 cm의 원형 다이아프램 중앙에 광섬유 Fabry-Perot 간섭계를 부착하여 광섬유의 스트레인 광학 효과를 이용하게 구성한 압력센서 1개를 센서 시스템에 연결하여 간섭형 광섬유 압력 센서 시스템을 구성하였다. 압력센서의 동작을 수조실험에서 확인함으로써 압력의 원격 측정이 가능함을 보였으며, 수조 실험의 길과 2 m의 측정범위에서 오차는 ${\pm}3.6\;cm$이내인 것으로 나타났다.

• 에너지공학
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• 제13권2호
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• pp.144-151
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• 2004

희박 예혼합 연소방식을 채용한 150MW급 대형 저 NOx 가스터빈 연소기에서 발생하는 급격한 연소진동 발생을 저감하였다. 희박 예혼합 연소기에서는 연소튜닝이 적절히 이루어지지 많은 경우에 연소불안정에 기인한 높은 연소진동의 발생과 함께 NOx 배출량이 높아질 가능성이 있다. 대상 가스터빈의 연소 모드 전환 중에 발생하는 연소진동의 주파수와 크기는 각각 80Hz및 4-9psi로 나타났으며, 대기온도가 낮아짐에 따라 연소진동의 크기가 증가하는 경향을 보였다. 연소진동에 영향을 미치는 인자로서 버너노즐로 공급되는 연료유량을 균등화하기 위한 연소튜닝과 연소모드 전환시 연료라인에 연료를 미리 공급(prefilling)하는 것이 화염안정에 매우 큰 효과가 있었다. 그 결과 연소모드 전환 중에 발생하는 연소진동을 2.5psi까지 저감할 수 있었으며, 150 MW기저부하 운전 중에 NOx 발생량을 35-43ppm(15% $O_2$)으로 유지할 수 있었다.

• 자원환경지질
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• 제25권3호
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• pp.283-296
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• 1992

The Keumryeong deposits is a low grade copper deposits in which copper minerals form disseminated grains and thin veinlets in felsic volcanics seem to be dacite. Alteration of the volcanics consists mainly pervasive propylitization and silicification. Potassic alteration characterized by biotite developed locally adjacent to southwestern contact of granodiorite body. Principal sulfide minerals in altered zone are mainly pyrite and lesser chalcopyrite. Chalcopyrite content in potassic zone is relatively higher than that of surrounding propylitized zone. Pyrite and chalcopyrite accompanies magnetite, molybdenite, sphalerite, pyrrhotite, arsenopyrite, pentlandite, marcasite, hematite, ilmenite, rutile, bismuthinite and native Bi as disseminations, veinlets and knots. Granodiorite body is propylitized and contains veinlets of pyrite, chalcopyrite and molybdenite. Fluid inclusions in sulfide-bearing quartz veinlets and quartz grains of felsic volcanics and granodiorite in altered zone consist of liquid-rich, vapor-rich, $CO_2-bearing$ and halite-bearing inclusions. These four types of inclusion intimately associated on a microscopic scale and indicate condensing or boiling of ore fluid during mineralization. Homogenization temperature of coexisting fluid inclusions are mostly in the range of 350 to $450^{\circ}C$. High salinity fluid contains 28.6 to 48.4 weight percent NaCI equivalent and moderate salinity fluid cotains 0.5 to 12.5 weight percent NaCl equivalent. Pressure estimated from $CO_2$ mole fraction of $CO_2-bearing$ inclusion range 160 to 375 bars. The Kigu copper deposits is a fissure filling copper vein developed 500 m south from the Keumryong deposits. Mineralogy and fluid inclusion data of the Kigu deposits are similar to that of the Keumryeong deposits. Homogenization temperature of fluid inclusions from the Kigu deposits are reasonable agreement with temperature estimated from sulfidation curve of cubanite-chalcopyrite-pyrite-pyrrhotite and pyrite-pyrrhotite mineral assemblages. Not only mineral occurrence and wall rock alteration in the Keumryeong deposits but also fluid inclusion data such as temperature, salinity, pressure and boiling evidences are similar to those of porphyry copper deposits.

• 한국표면공학회지
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• 제50권2호
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• pp.98-107
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• 2017

Pd-based membranes have been widely used in hydrogen purification and separation due to their high hydrogen diffusivity and infinite selectivity. However, it has been difficult to fabricate thin and dense Pd-based membranes on a porous stainless steel(PSS) support. In case of a conventional PSS support having the large size of surface pores, it was required to use complex surface treatment and thick Pd coating more than $6{\mu}m$ on the PSS was required in order to form pore free surface. In this study, we could fabricate thin and dense Pd membrane with only $3{\mu}m$ Pd layer on a new PSS support manufactured by metal injection molding(MIM). The PSS support had low surface roughness and mean pore size of $5{\mu}m$. Pd membrane were prepared by advanced Pd sputter deposition on the modified PSS support using fine polishing and YSZ vacuum filling surface treatment. At temperature $400^{\circ}C$ and transmembrane pressure difference of 1 bar, hydrogen flux and selectivity of $H_2/N_2$ were $11.22ml\;cm^{-2}min^{-1}$ and infinity, respectively. Comparing with $6{\mu}m$ Pd membrane, $3{\mu}m$ Pd membrane showed 2.5 times higher hydrogen flux which could be due to the decreased Pd layer thickness from $6{\mu}m$ to $3{\mu}m$ and an increased porosity. It was also found that pressure exponent was changed from 0.5 on $6{\mu}m$ Pd membrane to 0.8 on $3{\mu}m$ Pd membrane.

• Nuclear Engineering and Technology
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• 제12권3호
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• pp.163-170
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• 1980

4KJ의 에너지 뱅크(16.5KV, 35nH)를 사용하여 Mather형의 플라즈마총을 1 torr이하의 낮은 기체압력에서 동작시키면서 플라즈마의 효율적인 집속조건을 구하였다. 중수소기체의 충전압력이 0.18torr, 저장에너지가 3.8KJ일때 방전전류의 최고치는 180KA이었고 플라즈마의 축방향 평균속도는 약 $7cm/\mu\textrm{s}$이었다. 이것은 snowplow모델에 의해 계산된 속도보다 작은 값인데 이는 절연재 표면을 통한 전류의 손실에 기인하는 것으로 생각된다. H. Bruzzone의 플라즈마 집속장치(1KJ, 16KV, $4.2\mu\textrm{s}$)에 비해 본 실험에서는 기체압력이 낮은 역역에서 플라즈마 접속이 일어났다. 이는 이 실험에서 사용한 플라즈마총의 크기가 저장에너지에 비해 크고 또 잔여기체의 함량이 비교적 높기 때문이다. 집속된 플라즈마로 부터 방출되는 중성자는 Long counter를 사용해서 계측했다.

• 한국진공학회:학술대회논문집
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• 한국진공학회 1998년도 제14회 학술발표회 논문개요집
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• pp.77-77
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• 1998

Present silicon dioxide (SiOz) 떠m as intennetal dielectridIMD) layers will result in high parasitic c capacitance and crosstalk interference in 비gh density devices. Low dielectric materials such as f f1uorina뼈 silicon oxide(SiOF) and f1uoropolymer IMD layers have been tried to s이ve this problem. I In the SiOF ftlm, as fluorine concentration increases the dielectric constant of t뼈 film decreases but i it becomes unstable and wa않r absorptivity increases. The dielectric constant above 3.0 is obtain어 i in these ftlms. Fluoropolymers such as polyte$\sigma$따luoroethylene(PTFE) are known as low dielectric c constant (>2.0) materials. However, their $\alpha$)Or thermal stability and low adhesive fa$\pi$e have h hindered 야1리ru뚱 as IMD ma따"ials. 1 The concept of a plasma processing a찌Jaratus with 비gh density plasma at low pressure has r received much attention for deposition because films made in these plasma reactors have many a advantages such as go여 film quality and gap filling profile. High ion flux with low ion energy in m the high density plasma make the low contamination and go어 $\sigma$'Oss피lked ftlm. Especially the h helicon plasma reactor have attractive features for ftlm deposition 야~au똥 of i앙 high density plasma p production compared with other conventional type plasma soun:es. I In this pa야Jr, we present the results on the low dielectric constant fluorocarbonated-SiOF film d밑JOsited on p-Si(loo) 5 inch silicon substrates with 00% of 0dFTES gas mixture and 20% of Ar g gas in a helicon plasma reactor. High density 띠asma is generated in the conventional helicon p plasma soun:e with Nagoya type ill antenna, 5-15 MHz and 1 kW RF power, 700 Gauss of m magnetic field, and 1.5 mTorr of pressure. The electron density and temperature of the 0dFTES d discharge are measUI벼 by Langmuir probe. The relative density of radicals are measured by optic허 e emission spe따'Oscopy(OES). Chemical bonding structure 3I피 atomic concentration 따'C characterized u using fourier transform infrared(FTIR) s야3띠"Oscopy and X -ray photonelectron spl:’따'Oscopy (XPS). D Dielectric constant is measured using a metal insulator semiconductor (MIS;AVO.4 $\mu$ m thick f fIlmlp-SD s$\sigma$ucture. A chemical stoichiome$\sigma$y of 야Ie fluorocarbina$textsc{k}$영-SiOF film 따~si야영 at room temperature, which t the flow rate of Oz and FTES gas is Isccm and 6sccm, res야~tvely, is form려 야Ie SiouFo.36Co.14. A d dielec$\sigma$ic constant of this fIlm is 2.8, but the s$\alpha$'!Cimen at annealed 5OOt: is obtain려 3.24, and the s stepcoverage in the 0.4 $\mu$ m and 0.5 $\mu$ m pattern 킹'C above 92% and 91% without void, res야~tively. res야~tively.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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• pp.241.1-241.1
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• 2014

The large-area high-power radio-frequency (RF) driven ion sources based on the negative hydrogen (deuterium) ion beam extraction are the major components of neutral beam injection (NBI) systems in future large-scale fusion devices such as an ITER and DEMO. Positive hydrogen (deuterium) RF ion sources were the major components of the second NBI system on ASDEX-U tokamak. A test large-area high-power RF ion source (LAHP-RaFIS) has been developed for steady-state operation at the Korea Atomic Energy Research Institute (KAERI) to extract the positive ions, which can be used for the NBI heating and current drive systems in the present fusion devices, and to extract the negative ions for negative ion-based plasma heating and for future fusion devices such as a Fusion Neutron Source and Korea-DEMO. The test RF ion source consists of a driver region, including a helical antenna and a discharge chamber, and an expansion region. RF power can be transferred at up to 10 kW with a fixed frequency of 2 MHz through an optimized RF matching system. An actively water-cooled Faraday shield is located inside the driver region of the ion source for the stable and steady-state operations of RF discharge. The characteristics and uniformities of the plasma parameter in the RF ion source were measured at the lowest area of the expansion bucket using two RF-compensated electrostatic probes along the direction of the short- and long-dimensions of the expansion region. The plasma parameters in the expansion region were characterized by the variation of loaded RF power (voltage) and filling gas pressure.

• 한국건축시공학회지
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• 제15권2호
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• pp.201-207
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• 2015

본 연구에서는 고로슬래그 다량치환 콘크리트의 탄산화 저항성 및 내동해성 향상을 위하여 팽창성 인공 기포인 Expancel과 ERCO를 조합 사용하고 그에 따른 일련의 실험을 진행하고자 한다. 연구결과에 따르면 ERCO 치환에 따라 비누화반응에 의한 모세관공극 충전효과로 탄산화 저항성이 향상되었으며, 이 때 문제점으로 지적된 내동해성 저하현상을 개선하기 위하여 Expancel을 사용하였는데, Expancel 치환율이 증가함에 따라 내동해성이 대폭 개선되는 것으로 나타났다. 이는 Expancel이 외부압력에 의해 선택적으로 체적축소현상과 기포간격계수의 감소에 기인한 결과로 판단된다.

• Structural Engineering and Mechanics
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• 제91권1호
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• pp.75-86
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• 2024

In this paper, the porous metal PM-35 is proposed as the filler material of filled thin-walled tubes (FTTs), and a series of experimental study is conducted to investigate the dynamic behavior and energy absorption performance of PM-35 filled thin-walled tubes under impact loading. Firstly, cylinder solid specimens of PM-35 steel are tested to investigate the impact mechanical behavior by using the Split Hopkinson pressure bar set (SHP); Secondly, the filled thin-walled tube specimens with different geometric parameters are designed and tested to investigate the feasibility of PM-35 steel applied in FTTs by the orthogonal test. According to the results of this research, it is concluded that PM-35 steel is with the excellent characteristics of high energy absorption capacity and low yield strength, which make it a potential filler material for FTTs. The micron-sizes pore structure of PM-35 is the main reason for the macroscopic mechanical behavior of PM-35 steel under impact loading, which makes the material to exhibit greater deformation when subjected to external forces and obviously improve the toughness of the material. In addition, PM-35 steel core-filled thin-wall tube has excellent energy absorption ability under high-speed impact, which shows great application potential in the anti-collision structure facilities of high-speed railway and maglev train. The parameter V0 is most sensitive to the energy absorption of FTT specimens under impact loading, and the sensitivity order of different variations to the energy absorption is loading speed V0>D/t>D/L. The loading efficiency of the FTT is affected by its different geometry, which is mainly determined by the sleeve material and the filling material, which are not sensitive to changes in loading speed V0, D/t and D/L parameters.