• 터널과지하공간
• /
• 제17권5호
• /
• pp.372-380
• /
• 2007

침하로 인한 지표 손상대는 지하 채굴로 인해 발생되는 결과로서, 오랜 기간 동안 서서히 또는 급작스럽게 발생할 수 있다. 이러한 지표 손상대는 싱크홀 혹은 트러프형 침하에서 대규모 슬라딩에 이르기까지 다양한 형태로 관찰된다. 침하 발행 위험에 대한 평가는 광산 침하의 영향을 받는 지역에 있어서는 매우 중요하다. 이러한 위험도 평가나 침하 예측을 위해 경험적 모델, 프로파일함수, 영향 함수 그리고 수치해석과 같은 다양한 방법들이 적용되어 왔다. 본 연구에서는 다양한 인자들 중 지배적으로 침하 현상을 유발할 수 있는 채굴적과 관련한 정보, 즉 채굴적의 위치 및 규모의 정보를 확산이론과 연계한 비교적 간단한 침하 위험도 평가 기법을 제안하였다. 확산 모델은 지반 침하 기구를 설명할 수 있는 입자 모델과 상사관계를 가진다. 확산 모델을 폐금속광 및 폐석탄광 지역의 침하 위험도 작성에 적용하였다. 침하 위험도 평가를 위한 확산 모델은 매우 간단하지만 효율적인 방법임을 확인할 수 있었다.

• 한국방사선학회논문지
• /
• 제12권1호
• /
• pp.101-106
• /
• 2018

다층박막거울은 높은 반사 효율로 엑스선을 단색화 하는데 많이 사용되고 있다. 반사되는 엑스선의 파장은 두께주기와 입사각도에 의해 결정되고, 반사율은 층수와 표면 거칠기에 크게 의존하게 된다. 다층박막거울은 중원소와 경원소가 번갈아 적층되어 있는 구조로 되어 있으며 각 계면에서의 거칠기를 고려해야 한다. 본 논문에서는 두께 변화 W/Si 다층박막거울에서 계면 거칠기와 상호확산을 동시에 고려하여 반사율을 조사하였다. 두께 변화 다층박막거울은 균일한 다층박막거울에 비해 반사율은 감소하나 각도 및 에너지 반치폭이 넓은 특징을 보였으며, 상호확산에 따른 반사율의 저하가 크게 증가하였다. 이론적인 설계값에 가까운 반사율을 획득하기 위해서는 다층박막거울을 제작 할 때 나타나는 상호확산의 효과를 고려하여 설계함으로써 목적에 부합하는 최적의 다층박막거울을 설계하고 제작할 수 있을 것이다.

• 대한토목학회논문집
• /
• 제3권1호
• /
• pp.73-79
• /
• 1983

본(本) 연구(硏究)는 정수처리과정(淨水處理過程)의 하나인 염소처리(鹽素處理) 결과(結果) 생성(生成)되는 trihalomethane을 활성탄(活性炭)을 사용(使用)하여 흡착제거(吸着除去)할 때의 특성(特性)을 검토(檢討)하기 위한 실험(實驗)으로 증류수에 chloroform을 첨가하여 만든 인공시료(人工試料)를 가지고 5가지의 서로 다른 pH-온도(溫度)에 대한 등온흡착실험(等溫吸着實驗)과 회분실험(回分實驗) 실시하였다. 등온흡착실험(等溫吸着實驗) 결과(結果) 평형온도(平衡溫度)와 흡착량(吸着量) 사이의 관계(關係)는 Freundlich 식(式)을 적용(適用)할 수 있었고 온도(溫度)가 낮을수록 흡착량(吸着量)은 증가(增加)하였으며 pH가 흡착(吸着)에 미치는 효과(效果)는 무시(無視)할만 하였다. 회분흡착실험결과(回分吸着實驗結果)와 이론적(理輪的)인 모형(模型)의 simulation 결과(結果)로부터 계수(係數)를 산정(算定)하였으며 세공확산(細孔擴散)은 표면확산(表面擴散)에 비해 훨씬 빠른 것으로 나타났다.

• 한국재료학회지
• /
• 제25권4호
• /
• pp.202-208
• /
• 2015

Alumina dispersion strengthening copper(ADSC) alloy has great potential for use in many industrial applications such as contact supports, frictional break parts, electrode materials for lead wires, and spot welding with relatively high strength and good conductivity. In this study, we investigated the oxidation behavior of ADSC alloys. These alloys were fabricated in forms of plate and round type samples by surface oxidation reaction using Cu-0.8Al, Cu-0.4Al-0.4Ti, and Cu-0.6Al-0.4Ti(wt%) alloys. The alloys were oxidized at $980^{\circ}C$ for 1 h, 2 h, and 4 h in ambient atmosphere. The microstructure was observed with an optical microscope(OM) and a scanning electron microscope(SEM) equipped with energy-dispersive X-ray spectroscopy(EDS). Characterization of alumina was carried out using a 200 kV field-emission transmission electron microscope(TEM). As a result, various oxides including Ti were formed in the oxidation layer, in addition to ${\gamma}$-alumina. The thickness of the oxidation layer increased with Ti addition to the Cu-Al alloy and with the oxidation time. The corrected diffusion equation for the plate and round type samples showed different oxidation layer thickness under the same conditions. Diffusion length of the round type specimen had a value higher than that of its plate counterpart because the oxygen concentration per unit area of the round type specimen was higher than that of the plate type specimen at the same diffusion depth.

• 한국분말야금학회:학술대회논문집
• /
• 한국분말야금학회 2002년도 추계학술강연 및 발표대회
• /
• pp.8-8
• /
• 2002

TiC core/(Ti,Mo)C rim structure in TiC-$Mo_2C$-Ni base cermet which is generally prepared by sintering below 145$0^{\circ}C$ had been believed to be generated by the solid diffusion of Mo atoms 1 into TiC grains (D. Moskowitz and M.Humenik, 1r.:1966). Afterward, it was clarified that the c core/rim structure is generated by solution/re-precipitation mechanism : (1) $Mo_2C$ grains and s small TiC grains dissolve into the Ni liquid, (2) the dissolved Mo, Ti and C atoms migrate to the s surface of TiC coarse grains, (3) the Mo, Ti and C precipitate on the surface of TiC coarse g grains and form (Ti,Mo)C solid solution rim, and (4) the Ostwald ripening (grain growth by s solution/re-precipitation mechanism) of TiC-core/(Ti,Mo)-rim grains continues, and thus the w width of (Ti,Mo)C rim (at the same time, the grain size) increases with sintering time, etc. ( (H.Suzuki, K.Hayashi and O.Terada: 1973). The TiC-core was found not to disappear even by s sintering at 190$0^{\circ}C$ (ibid.: 1974) Recently, FeSi core/$Fe_2Si_5$-rim structure in Fe-66.7at%Si thermoelectric aIloy was found to also h hardly shrink and disappear by long heating at an appropriate temperature (1999: M.Tajima and K K.hayashD. Then, the authors considered its cause, and clarified experimentaIly that the disappearance of FeSi-core/$Fe_2Ski_5$-rim structure could be attributed to the exhaustion of diffusion-contributable vacancies in core/rim structure (N.Taniguchi and K.Hayashi:2001). At p present, the authors and my coworker are investigating whether the non-disappearance of TiC c core can be explained also from the new hypothesis "Exhaustion of diffusion-contributable v vacancies in corelrim structure".ure".uot;.

• 공업화학
• /
• 제19권2호
• /
• pp.236-241
• /
• 2008

자외선 조사에 따른 광촉매 $TiO_2$의 표면에서 발생하는 활성산소종의 기상확산을 이용하여 실리콘기판 위에 산화박막을 성장시켰다. 자외선의 세기, 기판의 온도와 반응기 내의 산소 압력을 공정변수로 한 결과, 일정두께의 실리콘 산화박막의 성장이 자외선의 세기가 증가할수록 빨랐으며, 자외선램프의 세기를 60 W BLB 램프에서 1 kW 고압수은 랩프로 변경할 경우 성장속도가 8배 정도 빨라졌다. 반응기 내의 압력이 증가할수록 실리콘 산화박막의 성장속도는 느렸다. 대부분 산화박막의 성장은 $20{\AA}$에서 포화되었으며, 자외선의 세기가 증가할수록 포화상태까지 도달시간이 빨라졌다. 성장된 산화박막을 열처리를 통하여 전형적인 열산화막의 물성에 도달할 수 있었다. 광활성 산소종의 기상확산은 실리콘 산화박막의 저온 형성에 대한 광촉매 활용이라는 새로운 산화공정 방법으로 사용이 가능함을 확인할 수 있었다.

• Journal of Applied Biological Chemistry
• /
• 제43권3호
• /
• pp.170-175
• /
• 2000

A pot-lysimeter experiment was conducted with 3-year-old 'Tsugaru' apple (Malus domestica Borkh) trees to examine the changes in oxygen diffusion rate (ODR) with lateral flow velocity of water through soil. The influence of lateral water flow velocity on water relations and elemental content in leaf, and sap temperature distribution patterns of the xylem of trees were also determined. Trees were grown under four soil water regimes: (1) fast laterally flowing (FWT, $2.50{\times}10^{-4}cm\;s^{-1}$), (2) slow laterally flowing (SWT, $0.25{\times}10^{-4}cm\;s^{-1}$), and (3) stagnant water table (WLT) at 60-cm, and (4) drip-irrigation at -40 kPa of soil matric potential as a control. The rate of $O_2$ diffusion converged near $2{\times}10^{-3}g\;m^{-2}\;min^{-1}$ for FWT and control soils, but decreased below $1{\times}10^{-3}g\;m^{-2}\;min^{-1}$ 40 days after treatment (DAT) for WLT soils. For SWT soils, however, the ODR at 15 cm below the soil surface was similar to that of control, but at 45 cm below the soil surface, ODR was similar to that of the WLT treatment. Leaf water potential of FWT and SWT plants was similar to that of control plants, but the values for SWT plants declined by 98 DAT. Leaf water potential of WLT plants decreased from -1.86 MPa (9 DAT) to -2.41 MPa (59 DAT) and finally down to -2.70 MPa. The sap temperature measured at 1100-hr was lowest at top and highest at bottom for FWT and control plants, but this pattern of SWT and WLT plants was disturbed from 29 DAT. However, for SWT plants, such thermal disturbance of sap temperature disappeared from 63 DAT.

• 한국분말야금학회:학술대회논문집
• /
• 한국분말야금학회 2006년도 Extended Abstracts of 2006 POWDER METALLURGY World Congress Part2
• /
• pp.1018-1021
• /
• 2006

Powdered metal parts and components may be carburized successfully in a vacuum furnace by combining carburizing technology $VacCarb^{TM}$ with a hi-tech control system. This approach is different from traditional carburizing methods, because vacuum carburizing is a non-equilibrium process. It is not possible to set the carbon potential as in a traditional carburizing atmosphere and control its composition in order to obtain a desired carburized case. This paper presents test results that demonstrate that vacuum carburizing system $VacCarb^{TM}$ carburized P.M. materials faster than traditional steel with acceptable results. In the experiments conducted, PM samples with the lowest density and open porosity showed a dramatic increase in the surface carbon content up to 2.5%C and a 3 times deeper case. Currently the boost-diffusion technique is applied to control the surface carbon content and distribution in the case. In the first boost step, the flow of the carburizing gas has to be sufficient to saturate the austenite, while avoiding soot deposition and formation of massive carbides. To accomplish this goal, the proper gas flow rate has to be calculated. In the case of P.M. parts, more carbon can be absorbed by the part's surface because of the additional internal surface area created by pores present in the carburized case. This amount will depend on the density of the part, the densification grade of the surface layer and the stage of the surface. "as machined" or "as sintered". It is believed that enhanced gas diffusion after initial evacuation of the P.M. parts leads to faster carburization from within the pores, especially when pores are open . surface "as sintered" and interconnected . low density. A serious problem with vacuum carburizing is delivery of the carbon in a uniform manner to the work pieces. This led to the development of the different methods of carburizing gas circulation such as the pulse/pump method or the pulse/pause technique applied in SECO/WARWICK's $VacCarb^{TM}$ Technology. In both cases, each pressure change may deliver fresh carburizing atmosphere into the pores and leads to faster carburization from within the pores. Since today's control of vacuum carburizing is based largely on empirical results, presented experiments may lead to better understanding and improved control of the process.

• 반도체디스플레이기술학회지
• /
• 제9권2호
• /
• pp.33-39
• /
• 2010

The moisture absorption properties such as diffusion coefficient and moisture content ratio of liquid type epoxy resin systems with the filler were investigated. Bisphenol A type and Bisphenol F type epoxy resin, Kayahard MCD as hardener and 2-methylimidazole as catalyst were used in these epoxy resin systems. The nano-sized spherical type fused silica as filler were used in order to study the moisture absorption properties of these liquid type epoxy encapsulant according to the change of filler size. The temperature of glass transition (Tg) of these epoxy resin systems was measured using Dynamic Scanning Calorimeter (DSC), and the moisture absorption properties of these epoxy resin systems according to the change of time were observed at $85^{\circ}C$ and 85% relative humidity condition using a thermo-hygrostat. The diffusion coefficients in these systems were calculated in terms of modified Crank equation based on Ficks' law. An increase of Tg and diffusion coefficient with filler size in these systems can be observed, which are attributed to the increase of free volume with Tg. The change of maximum moisture absorption ratio according to the filler size and filler content cannot be observed; however, the diffusion coefficients of these systems decreased with filler content. The diffusion via free volume is dominant in the epoxy resin systems with low nano-sized filler content; however, the diffusion with the interaction of absorption according the increase of the filler surface area is dominant in the liquid type epoxy encapsulant with high nano-sized filler content.

• 한국건설순환자원학회논문집
• /
• 제6권4호
• /
• pp.245-251
• /
• 2018

최근 구조물의 유지관리의 중요성이 부각되면서 자기치유 콘크리트 기술 분야의 연구가 활발히 이루어지고 있다. 이에 반해서 자기치유 성능을 평가하기 위한 척도는 부족한 실정이다. 균열폭을 측정하기 위한 방법으로 시각적인 방법이 1차적으로 사용되고 있으나 시편 내부의 균열폭을 관찰하기가 어려우며, 비균질한 균열특성으로 인해 표면에 대한 국부적인 측정만 할 수 있는 단점이 있다. 균열에 대한 간접적인 평가 방법으로 투수실험이 널리 활용되고 있지만 물의 점성으로 인한 문제가 있으며, 또한 실험 중 시편내부 물질의 용출될 가능성이 존재한다. 본 연구에서는 기체확산 특성을 활용한 균열폭 평가 방법을 제안하고자 하였다. 아크릴로 이상화된 직선균열을 제작하여 균열폭, 두께에 따른 시편의 확산계수를 분석하였다. 실험결과를 통하여 균열폭과 확산계수는 선형관계에 있음을 보였고, 두께와 확산계수는 역수의 관계에 있음을 증명하였다.