• 한국수자원학회논문집
• /
• 제50권1호
• /
• pp.55-64
• /
• 2017

본 연구에서는 ULTIMATE 기법을 이용하여 밀도류 층적분 모형의 해석을 위한 수치모형을 제시하였다. 개발된 모형을 경사부와 평탄부로 이루어진 실내 실험에 적용하여 경사부에 유입된 부유사 밀도류의 전파 특성에 대해 분석하였다. ULTIMATE 기법의 범용제한자로 인하여 밀도류의 선단부가 수치진동 없이 비교적 급한 형태로 전파되는 것을 모의하였다. 그리고 사류로 전파되고 수로 끝에서부터 상류로 변화되는 밀도류의 내부 도수 발생 과정을 재현하였다. 이러한 내부 도수는 ULTIMATE 제한자를 사용하면 Courant 수가 1 미만일 때 안정적으로 모의되는 것을 확인하였다. 또한 밀도류의 전파 속도에 영향을 주는 인자에 대하여 분석하였다. 입자의 크기는 $9{\mu}m$ 이하일 때 밀도류의 전파 속도에 큰 영향을 주지 않는 반면, 부력 흐름률은 확연한 영향을 주는 것을 확인하였다. 마지막으로 부유사 밀도류에 의한 하상변동에 대해 검토하였다. 수치모형으로 부유사 밀도류의 전파에 의한 하상변동을 정량적으로 적절히 모의하였으며, 도수로 인한 부유사 연행의 차이와 이로 인한 하상의 불연속적인 형태를 관찰할 수 있었다.

• 환경영향평가
• /
• 제25권3호
• /
• pp.209-221
• /
• 2016

관인취수장의 취수원은 하천기준으로 관련규정에 따라 취수지점으로부터 한탄강 상류 2.6km를 상수원보호구역으로 설정하여 각종 행위를 제한하고 있다. 그러나 관인취수장의 취수원이 하천수가 아닌 지하수를 취수하고 있으므로 현재 설정된 상수원보호구역과 상류의 각종 행위제한구역을 변경하여야 한다는 주장이 지속적으로 제기되었다. 이 연구에서는 이러한 주장을 검증하기 위해 수리지질 및 수리지구 화학조사를 실시하여 관인취수장의 취수원과 오염물질 유입특성을 평가했다. 관인취수장의 주변 지역은 화강암을 기반암으로 하여 상부에 총 4매의 제4기 현무암이 약 50m 두께로 충진 되어 있음을 확인하였다. 현무암 하부층은 낮은 비저항이고 화강암은 높은 비저항을 보여 현무암 하부층에 투수성 대수층이 존재하고 있는 것으로 보인다. 관인 취수장 유출량을 고려할 때 함양지역 면적은 최소 $5.7km^2$로 산정되었으며, 철원평야 일원에서 함양된 지하수가 대수층을 따라 흐르다 취수장 인근의 현무암과 화강암 부정합면을 따라 용출되는 것으로 추정되었다. 수리지구화학 조사 결과 관인취수장 용천수는 현무암대수층 지하수와 유사하고, $SiO_2$, Mg, $NO_3$, $SO_4$를 포함하는 주요 용존 화학성분의 시기적 농도 변동도 취수장 용천수는 현무암대수층에서 유래되었음이 밝혀졌다. 결론적으로 수리지질학적 및 수리지구화학적 특성으로 볼 때 관인취수장 용천수는 하천수나 저수지수는 아니고 현무암대수층 지하수와 동일한 것으로 추정되었다.

• 대한기계학회논문집B
• /
• 제28권8호
• /
• pp.895-901
• /
• 2004

Single-phase convection and nucleate boiling heat transfer were locally investigated for confined planar water jets. The detailed distributions of the wall temperature and the convection coefficient as well as the typical boiling curves were discussed. The curve for the single-phase convection indicated the developing laminar boundary layer, accompanied by monotonic increase of the wall temperature in the stream direction. Boiling was initiated from the furthest downstream as heat flux increased. Heat transfer variation according to the streamwise location was reduced as heat flux increased enough to create the vigorous nucleate boiling. Velocity effects were considered for the confined free-surface jet. Higher velocity of the jet caused the boiling incipient to be delayed more. The transition to turbulence precipitated by the bubble-induced disturbance was obvious only for the highest velocity, which enabled the boiling incipient to start in the middle of the heated surface, rather than the furthest downstream as was the case of the moderate and low velocities. The temperature at offset line were somewhat tower than those at the centerline for single-phase convection and partial boiling, and these differences were reduced as the nucleate boiling developed. For the region prior to transition, the convection coefficient distributions were similar in both cases while the temperatures were somewhat lower in the submerged jet. For single-phase convection, transition was initiated at $x/W{\cong}2.5$ and completed soon for the submerged jet, but the onset of transition was retarded to the distance at $x/W{\cong}6$ for the fee-surface jet.

• Journal of Welding and Joining
• /
• 제34권1호
• /
• pp.75-81
• /
• 2016

This study applied laser surface melting process using CW(Continuous wave) Yb:YAG laser and cold-work die steel SM45C and investigated microstructure and hardness. Laser beam speed, power and beam interval are fixed at 70 mm/sec, 2.8 kW and $800{\mu}m$ respectively. Depth of Hardening layer(Melting zone) was a minimum of 0.8 mm and a maximum of 1.0 mm that exceeds the limit of minimum depth 0.5 mm applying trimming die. In all weld zone, macrostructure was dendrite structure. At the dendrite boundary, Mn, Al, S and O was segregated and MnS and Al oxide existed. However, this inclusion didn't observe in the heat-affected zone (HAZ). As a result of interpreting phase transformation of binary diagram, MnS crystallizes from liquid. Also, it estimated that Al oxide forms by reacting with oxygen in the atmosphere. The hardness of the melting zone was from 650 Hv to 660 Hv regardless of the location that higher 60 Hv than the hardness of the HAZ that had maximum 600 Hv. In comparison with the size of microstructure using electron backscatter diffraction(EBSD), the size of microstructure in the melting zone was smaller than HAZ. Because it estimated that cooling rate of laser surface melting process is faster than water quenching.

• 한국해양공학회지
• /
• 제26권4호
• /
• pp.50-56
• /
• 2012

When a liquid cargo tank is partially filled with fluid, internal impact loads can be occurred from the vessel's motions. In this study, liquid sloshing problems with a thin top layer of particles with a lighter density than water and the coupling effects of the liquid-sloshing/vessel-motion were investigated in order to reduce the sloshing-induced impact loads. The PNU-MPS (Pusan-National-University-modified Moving Particle Simulation) method for solving the liquid motion inside a tank and the CHARM3D BEM (Boundary Element Method) based time-domain ship motion analysis program for vessel-motion simulation were coupled. From the simulation results, we could see that the floaters seemed to be quite effective at reducing the sloshing impact loads in the case of tank-only sloshing problems, but not as much for the coupling problem with vessel motion.

• Journal of Advanced Marine Engineering and Technology
• /
• 제35권5호
• /
• pp.632-639
• /
• 2011

해양 파력 발전 시스템의 설계를 위하여 본 연구에서는 6-자유도운동해석 기법을 적용한 3차원 CFD 해석으로 두 개의 부유체에 대한 거동을 유입되는 파의 성질에 따라 해석하였다. 수조모델내에서의 파의 생성형상을 현재 실험에서 가장 많이 사용되는 피스톤 형식의 조파기와 동일한 형태의 파를 생성하였으나 얕은 수심으로 인하여 바닥면에서 생성되는 에크만 경계층에 의해 파의 에너지가 감쇄되는 현상을 보였다. 생성된 파를 이용하여 파장에 따른 부유체의 거동을 계산한 결과 파장이 5m인 경우 부유체의 최대 진폭은 0.3m, 파장 1m인 경우 최소 진폭은 0.15m 그리고 파장 6m인 경우 부유체간 최대 거리는 1.06m로 계산되었다.

• 한국항공우주학회지
• /
• 제31권6호
• /
• pp.88-95
• /
• 2003

임의의 성분비로 혼합되어 있는 CO$_2$와 H$_2$O 혼합가스에 대하여 회색가스가중합법(WSGGM)을 적용하였다. 모델의 타당성을 검증하기 위하여 두 가지 다른 형태의 문제를 고려하였다. 첫 번째는 문제는 일정한 분압하의 균일, 포물선 및 경계층 온도 분포를 갖는 매체에 대한 문제이고, 두 번째는 온도 및 분압이 일정치 않은 매체에 대한 문제이다. 고려된 두가지 형태의 문제들에 대하여 WSGGM을 이용한 결과는 기준이 되는 좁은밴드 모델(SNB)의 결과와 잘 일치하고 있는 것을 확인하였다. 본 연구에서 제안된 모델과 데이터베이스는 연소가스에 의한 복사열전달의 해석에 유용하게 사용될 수 있을 것이다.

• Ocean and Polar Research
• /
• 제26권2호
• /
• pp.145-154
• /
• 2004

Surface energy and $CO_2$ fluxes have been measured over an ocean at Ieodo Ocean Research Station of KORDI since May 2003. Eddy covariance technique, which is a direct flux measurement, is used to quantitatively understand the interaction between the ocean surface and the atmospheric boundary layer. Although fluxes were continuously measured during the period from May 2003 to February 2004, the quality control of these data yielded <20% of data retrieval. The atmospheric stability did not show any distinct dirunal patterns and remained near-neutral to stable from May to June but mostly unstable during fall and winter in 2003. Sensible heat flux showed a good correlation with the difference between the sea water temperature and the air temperature. The maximum fluxes of sensible heat and latent heat were $120Wm^{-2}$ and $350Wm^{-2}$ respectively, with an averaged Bowen ratio of 0.2. The ocean around the tower absorbed $CO_2$ from the atmosphere and the uptake rates showed seasonal variations. Based our preliminary results, the daytime $CO_2$ flux was steady with an average of $-0.1 mgCO_2m^{-2}s^{-1}$ in summer and increased in winter. The nighttime $CO_2$ uptake was greater and fluctuating, reaching up to $-0.1 mgCO_2m^{-2}s^{-1}$ but these data require further examination due to weak turbulent mixing at nighttime. The magnitude of $CO_2$ flux was positively correlated with the half hourly changes in horizontal mean wind speed. Due to the paucity of quality data, further data collection is needed for more detailed analyses and interpretation.

• 한국대기환경학회지
• /
• 제13권2호
• /
• pp.161-170
• /
• 1997

The concentrations of dimethylsulfide (DMS) were determined using samples collected from a station located at Kosan, Cheju Island during two field campaigns held in December 1996 and January 1997. The atmospheric DMS concentrations measured at 6-hr intervals during the entire campaign periods, after excluding a few extreme values, spanned in the range of 14 to 410 pptv with mean and 1 SD value of 127 $\pm$ 94 pptv (N=42). Between two month periods during which the field campaigns were conducted, a notable reduction in DMS levels was observed which was comparable to the dramatic shift in air temperature. A considerable difference was also noted in DMS levels, when data were grouped by day/night basis. The cause of unexpected, high day-to-night DMS ratios is best explained in terms of high efficiency of daytime source processes relative to low efficiency of nighttime sink processes due to the characteristics of the study location. The surface water DMS of the study site, although scarcely measured, also behaved similarly to its atmospheric counterpart with its range from 0.3 to 19 nM (N=11). When correlation analysis was conducted between the atmospheric DMS concentration and other concurrently determined parameters, significant correlations were observed from most basic meteorological parameters such as windspeed, relative humidy, and air temperature. However, the existence of "not-so-strong" correlations between air temperature and DMS concentrations relative to other ones indicated that the effect of temperature on DMS behavior must be reflected in more complicated manners at the study site. The sea-to-air flux of DMS was approximated through an application of the mass-balance flux calculation method of Wylie and de Mora (1996) under the assumption that sink mechanism within the marine boundary layer is in steady-state condition with its counterpart, source mechanism. Based on this estimation method, we reached a conclusion that oceanic DMS emitted from the southwest sea of the Korean Peninsula can amount to approximately 9 $\sim$ 36 Gg S $yr^{-1}$.$yr^{-1}$.

• 한국지반공학회:학술대회논문집
• /
• 한국지반공학회 2005년도 춘계 학술발표회 논문집
• /
• pp.107-112
• /
• 2005

Road is built continuously along with development of industry and cut slope is happened necessarily in road construction. Geoengineers are executing cut slope stability analysis considering various cut slope condition such as topography, geology, hydraulic condition and so on. The Tertiary Jungja Basin is located in the southeastern coastal area of the Korea Peninsula. Jungja Basin area is created by geotectonic movement of the plate after Early Miocene epoch. The northwestern and southwestern boundary of the basin is fault zone. The Basement rock is hornfels (Ulsan Formation). Basin-fills consist of extrusive volcanic rock(Tangsa Andesites), unconsolidated fluviatile conglomerate(Kangdong Formation) and shallow brackish-water sandstone(Sinhyun Formation). The characteristics of cut slopes in this area is different with cut slopes in the other site. Soil layers in this area is unconsolidated sediments and is not formed the weathering and erosion of the rock. So, the depth of soil layer is very thick. Faults of this area are northwest-southeast and northeast-southwest direction. Expandible clay mineral as smectite, chlorite et al. detected from fault gouge using XRD. Therefore, Jungja Basin area must consider the characteristics of the faults and soil layers thickness necessarily cut slopes stability analysis.