• 한국물환경학회지
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• 제33권4호
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• pp.449-459
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• 2017

In Geum River of Korea, three multi-purpose weirs were built at the downstream of Daecheong Reservoir during the Four Major River Restoration Project (FMRRP). The weirs have altered the hydraulic characteristics of the river, and consequently transformed the large areas of flowing ecosystem to deep and wide stagnant environment. In every summer, a thermal stratification occurred near the Baekje Weir having mean depth of 4.0 m, and the surface algal blooms dominated by buoyant cyanobacteria have been frequently formed after the FMRRP. The objective of this study was to investigate the relationship between flow velocity and thermal stability of the waterbody using a three-dimensional (3D) hydrodynamic model (EFDC+) after calibration against the thermistor chain data obtained in 2014. A new Sigma-Zed vertical grid system of EFDC+ that minimize the pressure gradient errors was used to better simulate the thermodynamics of the waterbody. The model reasonably simulated the vertical profiles of the observed water temperatures. The vertical mean flow velocity and the Richardson Number (Ri) that represents the stability of waterbody were estimated for various management water levels and flow rates scenarios. The results indicated that the thermal stability of the waterbody is mostly high ($Ri{\gg}0.25$) enough to establish stratification, and largely depend on the flow velocity. The critical flow velocity that can avoid a persistent thermal stratification was found to be approximately 0.1 m/s.

• 태양에너지
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• 제7권2호
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• pp.22-29
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• 1987

This paper dealed with thickness variation of bottom heat sotrage zone due to salinity and flow rate of extration hot brine in small test solar pond (0.5m wide, 0.5m high, 1.0m long). Testing apparatus and situation were follows: 7.1 cm of height of suction diffuser and 1.8cm of height of discharge diffuser above the test pond respectively, 0.3cm of slot size of suction diffuser, 1.0cm of slot size of discharge diffuser, 47cm of length of the slot; heating of hot water ($75^{\circ}C$) through separated hot water tank, discharge of the brine into storage zone through discharge diffuser, the extration of the brine through suction diffuser, circulation of the extracted brine through a heat exchanger (cooler). Following results were obtained through the experiments. 1. In small test solar pond, the typical three zone which showed up in real solar pond were established. 2. Richardson Number was used more effectively to confirm hydrodynamic stability of the stratified flow. 3. The thickness of non convective layer had a great effect on the heat storage of the bottom convective layer, then the temperature of bottom convective layer had a relation to that of upper convective layer. 4. Optimum operating condition in the test pond was on 10%-15% of salt concentration and $0.05m^3/hr$ of flow rate of extraction hot brine. 5. Following thickness of 3 zones were available to obtain under optimum operation condition: o bottom storage zone: $30%{\pm}10%$ of total pond depth o non-convective zone: $40%{\pm}10%$ of total pond depth o Upper surface zone: $20%{\pm}10%$ of total pond depth.

• Environmental Sciences Bulletin of The Korean Environmental Sciences Society
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• 제1권1호
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• pp.35-43
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• 1997

Handling the emergency problems such as Chemobyl accident require real time prediction of pollutants dispersion. One-point real time sounding at pollutant source and simple model including turbulent-radiation process are very important to predict dispersion at real time. The stability categories obtained by one-dimensional numerical model (including PBL dynamics and radiative process) are good agreement with observational data (Golder, 1972). Therefore, the meteorological parameters (thermal, moisture and momentum fluxes; sensible and latent heat; Monin-Obukhov length and bulk Richardson number; vertical diffusion coefficient and TKE; mixing height) calculated by this model will be useful to understand the structure of stable boundary layer and to handling the emergency problems such as dangerous gasses accident. Especially, this simple model has strong merit for practical dispersion models which require turbulence process but does not takes long time to real predictions. According to the results of this model, the urban area has stronger vertical dispersion and weaker horizontal dispersion than rural area during daytime in summer season. The maximum stability class of urban area and rural area are 'A' and 'B' at 14 LST, respectively. After 20 LST, both urban and rural area have weak vertical dispersion, but they have strong horizontal dispersion. Generally, the urban area have larger radius of horizontal dispersion than rural area. Considering the resolution and time consuming problems of three dimensional grid model, one-dimensional model with one-point real sounding have strong merit for practical dispersion model.

• Nuclear Engineering and Technology
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• 제51권4호
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• pp.987-995
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• 2019

Steam jet condensation is of great importance to pressure suppression containment and automatic depressurization system in nuclear power plant. In this paper, the condensation processes of sonic steam jet in a quiescent subcooled pool are recorded and analyzed, more precise understanding are got in direct contact condensation. Experiments are conducted at atmospheric pressure, and the steam is injected into the subcooled water pool through a vertical nozzle with the inner diameter of 10 mm, water temperature in the range of $25-60^{\circ}C$ and mass velocity in the range of $320-1080kg/m^2s$. Richardson number is calculated based on the conservation of momentum for single water jet and its values are in the range of 0.16-2.67. There is no thermal stratification observed in the water pool. Four condensation regimes are observed, including condensation oscillation, contraction, expansion-contraction and double expansion-contraction shapes. A condensation regime map is present based on steam mass velocity and water temperature. The dimensionless steam plume length increase with the increase of steam mass velocity and water temperature, and its values are in the range of 1.4-9.0. Condensation heat transfer coefficient decreases with the increase of steam mass velocity and water temperature, and its values are in the range of $1.44-3.65MW/m^2^{\circ}C$. New more accurate semi-empirical correlations for prediction of the dimensionless steam plume length and condensation heat transfer coefficient are proposed respectively. The discrepancy of predicted plume length is within ${\pm}10%$ for present experimental results and ${\pm}25%$ for previous researchers. The discrepancy of predicted condensation heat transfer coefficient is with ${\pm}12%$.

• Wind and Structures
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• 제36권3호
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• pp.201-213
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• 2023

In this study, the effect of sea surface temperature (SST) on the distribution of vertical wind speed in the atmospheric boundary layer of coastal areas was analyzed. In general, coastal areas are known to be more susceptible to various meteorological factors than inland areas due to interannual changes in sea surface temperature. Therefore, the purpose of this study is to analyze the relationship between sea surface temperature (ERA5) and wind resource data based on the meteorological mast of Høvsøre, the test bed area of the onshore wind farm in the coastal area of Denmark. In addition, the possibility of coastal disasters caused by abnormal vertical wind shear due to changes in sea surface temperature was also analyzed. According to the analysis of the correlation between the wind resource data at met mast and the sea surface temperature by ERA5, the wind speed from the sea and the vertical wind shear are stronger than from the inland, and are vulnerable to seasonal sea surface temperature fluctuations. In particular, the abnormal vertical wind shear, in which only the lower wind speed was strengthened and appeared in the form of a nose, mainly appeared in winter when the atmosphere was near-neutral or stable, and all occurred when the wind blows from the sea. This phenomenon usually occurred when there was a sudden change in sea surface temperature within a short period of time.

• 한국해양학회지:바다
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• 제19권3호
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• pp.180-190
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• 2014

연안에서 관측된 Acoustic Doppler Current Profiler(ADCP) 유속자료의 10-20%는 음향반사 측면효과로 인하여 일반적으로 사용하지 않는다. 본 연구는 ADCP의 사용되지 않았던 자료를 복구하여 영산강 하구에서 저조시 방류되는 담수의 경계면 이류속도를 구하고 이를 통해 담수 유량과 수층의 역학적 안정도를 보다 정확하게 계산하여 하구 내 혼합 환경을 잘 이해하고자 한다. 현장관측은 2011년 8월 영산강의 하구언 전면과 고하도 부근 두 정점에서 한달 동안 실시하였으며, 방류수의 이류속도는 유효 유속 판정에 상관도, 퍼센트굿, 그리고 유속 히스토그램의 엄격한 기준을 적용한 ADCP 후처리방법을 적용하여 복원하였다. 또한, 같은 수로에 위치한 두 정점에서 이류하는 퇴적물의 농도피크시간을 토대로 퇴적물의 이류속도(Sediment Advection Speed)를 계산하여 방류수 이류속도를 비교 검증하였다. 퇴적물의 이류속도를 방류시 ADCP의 표층유속과 비교하였을 때, 방류량이 $2.0{\times}10^7$톤 보다 크면 두 속도값이 유사하고, 그보다 적을 경우에는 퇴적물의 이류속도가 약간 크게 산정되는 것을 볼 수 있었다. 방류가 발생할때 담수이류속도(Freshwater Advection Speed)는 바닥으로부터 $0.8{\times}$수심의 유속보다 평균 0.8 m/s 정도 크기 때문에, 방류가 증가하는 시기에 새롭게 계산된 방류수의 속도를 포함한 순유출량(=수심 및 조석주기로 적분된 흐름)을 계산하면, 그 방향이 하구언으로 들어오는 방향에서 빠져나가는 방향으로 바뀌는 것을 확인할 수 있었다. 또한, 표층 담수의 속도가 더해짐으로써 표층 속도쉬어와 리차드슨 수의 분포가 바뀜을 관찰할 수 있었기 때문에 표층 해수의 안정도를 해석함에 있어 실제 방류수 유속의 중요성을 알 수 있었다. 향후 유속과 함께 수온과 염분의 장기적인 관측이 수행된다면 담수 방류에 따른 성층의 생성과 소멸, 그리고 관련 부유퇴적물의 변동에 대해서도 보다 정확하게 파악할 수 있을 것으로 생각된다.

• 한국해양학회지:바다
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• 제8권3호
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• pp.307-316
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• 2003

천해 내만 해역인 남해 서부의 도암만 어류군집 조성을 조사하기 위하여 2001년 3월부터 2002년 2월까지 조망어구(beam trawl)를 이용하여 매월 중순경 최간조시에 어류를 채집하였다. 조사기간동안 총 33과 53종의 어류가 채집되었다. 도화망둑(Chaeturichthys hexanema), 주둥치(Leiognathus muchalis), 문절망둑(Acanthogobius flavimanus)의 3종이 전체 채질개체수의 67.4％를 차지하였으며, 생체량에서는 꼼치(Liparis tanakai), 문절망둑(Acanthogobius flavimanus), 도화망둑(Chaeturichthys hexanema)이 50.8％를 차지하는 우점종이었다. 채집 개체수와 생체량은 가을과 겨울에는 상대적으로 높게 나타났던 반면, 출현종수와 다양도 등의 일변량 지수값들은 대체로 봄과 여름에 높았다. 주요 14종의 월별 출현빈도에 의한 종간 집괴분석 결과 이 해역의 어류군집이 계절별로 출현양상을 달리하는 3개의 무리로 구분될 수 있음을 보였다: 1)계절에 관계없이 연중 출현하는 주거종에 속하는 도화망둑, 문절망둑, 개서대(Cynoglossus robustus) 및 반지(Setipinna taty)와 가을에 높은 출현 빈도를 보인 비늘양태(Onigocia spinosa), 돛양태 (Repomucenus lunatus), 주둥치, 2) 여름에 높은 출현빈도를 보인 노랑촉수(Upeneus japonicus), 갈치 (Trichiurus lepturus) 및 실망둑(Cryptocentrus filifer), 3) 겨울과 봄에 주로 출현하는 종으로 꼼치(Liparis tanakai), 풀미역치(Erisphex pottii), 두줄망둑(Tridentiger trigonocephalus) 및 동갈양태 (Repomucenus richardsottii). 어류군집의 계절에 따른 뚜렷한 분리는 나타나지 않았는데, 이와 같은 결과는 회유종들의 계절에 따른 일시 출현이 나타난다 하더라도, 전체 어류군집 조성이 출현 개체수에서 높은 점유율을 보이는 주거종에 의해 크게 지배를 받아 비교적 안정된 군집을 형성하고 있음을 시사하였다.

• 해양환경안전학회지
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• 제26권1호
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• pp.65-74
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• 2020

본 연구에서는 당동만을 중심으로 빈산소가 발생하는 물리적 해양환경 특성을 파악하고, 로지스틱 회귀분석을 이용해 빈산소 발생확률을 예측하였다. 관측 자료를 분석한 결과, 브런트-바이살라 주파수는 수심이 깊은 만 입구보다 수심이 얕은 만 내측에서 더 크게 나타났다. 이는 당동만 내측에서 담수 유입으로 인해 표층 염분이 낮아져 강한 밀도 성층이 형성되었기 때문이다. 시간적으로는 6월 ~ 9월까지 리차드슨 수와 브런트 바이살라 주파수가 매우 높게 나타났고, 9월 2일 이후로는 성층이 완화되어 감소하는 경향을 보였다. 당동만에서 관측된 용존산소 및 수온, 염분 자료를 분석한 결과, 저층의 용존산소 농도는 공통적으로 표층과 저층의 수온차에 가장 큰 영향을 받는 것으로 나타났다. 한편, 수심차(dz)를 고정된 변수로 두고, 수온차(dt)의 변화에 의한 빈산소의 발생 확률의 변화를 계산한 결과, 수심차(dz)가 각각 5 m, 10 m, 15 m, 20 m일 경우, 수온차(dt)는 8℃, 7℃, 5℃, 3℃일 때 빈산소 발생확률이 70 %를 상회하는 것으로 나타났다. 이는 당동만에서 수심차(dz)가 커질수록 빈산소 발생에 필요한 수온차(dt)는 작아지게 된다는 것을 뜻하며, 특히 당동만에서 수심차(dz)가 20 m 내외인 지역은 빈산소가 발생하기 매우 쉬운 환경이라는 것을 알 수 있었다.

• 대기
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• 제28권4호
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• pp.369-382
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• 2018

Planetary boundary layer height (PBLH), produced by the Local Data Assimilation and Prediction System (LDAPS), was verified using RawinSonde (RS) data obtained from observation at Daegwallyeong (DGW) and Sokcho (SCW) during the International Collaborative Experiments for Pyeongchang 2018 Olympic and Paralympic winter games (ICE-POP 2018). The PBLH was calculated using RS data by applying the bulk Richardson number and the parcel method. This calculated PBLH was then compared to the values produced by LDAPS. The PBLH simulations for DGW and SCW were generally underestimation. However, the PBLH was an overestimation from surface to 200 m and 450 m at DGW and SCW, respectively; this result of model's failure to correctly simulate the Surface Boundary Layer (SBL) and the Mixing Layer (ML) as the PBLH. When the accuracy of the PBLH simulation is low, large errors are seen in the mid- and low-level humidity. The highest frequencies of Planetary boundary layer (PBL) types, calculated by the LDAPS at DGW and SCW, were presented as types Ι and II, respectively. Analysis of meteorological factors according to the PBL types indicate that the PBLH of the existing stratocumulus were overestimated when the mid- and low-level humidity errors were large. If the instabilities of the surface and vertical mixing into clouds are considered important factors affecting the estimation of PBLH into model, then mid- and low-level humidity should also be considered important factors influencing PBLH simulation performance.