• 자원환경지질
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• 제9권1호
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• pp.27-43
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• 1976

The flourite in Hwacheon, Hwanggangri and Keumsan district are major fluorite producing areas in Korea. The fluorite deposits of Hwacheon district are wholly fissure filling hydrothermal veins embedded in Precambrian gneiss and schists and Jurassic granites. Also some fluorite deposits are emplaced in felsite whose age is unknown. Emplacement of most fluorite veins of the district are controlled by EW fracture system. Fluorites are generally accompanied to chalcedonic quartz and also kaolinite, montmorillonite, dickite and calcite in parts. Vertical and lateral mineral zonings are not distinct. The fluorite deposits in the Hwanggangri district are wholly embedded in limestone and other calcareous sediments of Paleozoic Yeongweol Group. Most of the fluorite deposits belong to one of two categories which are steeply. dipping veins and gently dipping replacement deposits adjacent to Late Cretaceous(83-90mys) granite bodies. The strikes of fluorite veins of Hwanggangri district mostly occupy the fractures of $N30^{\circ}-40^{\circ}E$ and $N30^{\circ}-40^{\circ}W$ system. Fluorites are accompanied to calcite, milky quartz, chalcedonic quartz, and also montmorillonite, kaolinite in parts. But in some deposits, scheelite, various sulfide minerals and barite are accompanied. Emplacement of fluorite deposits are largely controlled by lithology and structures of this district. In some deposits fluorite veins gradate to scheelite veins and also telescoping of the mineral zones are found in this district. In the Keumsan district, fissure-filled fluorite veins and replacement deposits are mostly emplaced in limestone of Paleozoic Yeongweol Group, late Cretaceous quartz-porphyry, granite and sandstone. Some deposits are emplaced in Precambrian metasediments. Mineralogy and other characteristics of the deposits in this district is similar to those of Hwanggangri district. Fluid inclusion studies reveal the difference of salinities, $CO_2$ contents of ore fluid and temperatures during fluorite mineral deposition in the these districts. In Hwacheon district, ore-fluids were comparatively dilute brine and low $CO_2$ content. Filling temperatures ranges $104^{\circ}C$ to $170^{\circ}C$. In the Chuncheonshinpo mine, most deeply exploited one in this district, salinitles range 0.5-2. 2wt. % NaCl and filling temperatures range from $116^{\circ}C$ to $143^{\circ}C$. In the Hwanggangri district, ore fluids were complex and filling temperature ranges very widly. In the contact metasomatic fluorite deposits, ore fluid were NaCl rich brines with moderate $CO_2$ content and filling temperatures range from $285^{\circ}C$ to above $360^{\circ}C$. Fluids inclusions in tungsten and sulfide minerals bearing fluorite veins show high $CO_2$ content up to 31wt. %. Filling temperature ranges from $101^{\circ}C$ to $310^{\circ}C$. Fluids inclusions In mainly fluorite bearing veins were more dilute brine and low $CO_2$ contents. Filling temperatures range from $95^{\circ}C$ to $312^{\circ}C$. Filling temperature of fluid inclusions of Keumsan district are between $95^{\circ}C$ and $237^{\circ}C$. Data gathered from geologic, mineralogic and fluid inclusion studies reveal that fluorite mineralization in H wacheon district proceeded at low temperature with dilute brine and low $CO_2$ content. In Hwangganri district, fluorite mineralization proceeded by several pulse of chemically distinct ore fluids and formed the mineralogically different type of deposits around cooling granite pluton which emplaced comparatively shallow depth.

• 자원환경지질
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• 제20권2호
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• pp.97-106
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• 1987

The geology of the Bupyeong mine area is consisted of Precambrian Gyeonggi gneiss complex and Mesozoic igneous rocks; i.e., pyroclastic rocks, intrusive breccia, granite and felsic porphyries which were formed during a Jurassic to early Cretaceous resurgent caldera evolution. Granites are not observed on the surface and in the underground of the mine. Bupyeong silver deposits occur as stockworks of base metal sulfides- minor silver minerals-quartz - carbonate veinlets, hosted by pyroclastic rocks and intrusive breccia at the southwestern margin of the caldera. Silver occurs mainly as native silver, and other silver minerals, minor in quantity, are argentite, tetrahedrite-freibergite, pyrargyrite, polybasite, canfieldite and dyscrasite. The average grade of silver ore is about 180g/t Ag. Discrimination of silver ore from the country rocks depends largely on the chemical analyses of rock samples taken every two meters from tunnels, diamond-drilling cores and mining stopes, because silver minerals are hardly observed in the ore by crude eye, and silver orebodies do not properly coincide with the concentrated zone of base metal sulfides which were precipitated at the earlier stage than the stage of precipitation of native silver. General characteristics of the loci of the silver orebodies are as follows; (1) The host rocks of orebodies are pyroclastic rocks and intrusive breccia. (2) Many of the orebodies are distributed around Gyeonggi gneiss complex. Especially where the paleotopography of gneiss complex shows a gradual slope, the basal stratigraphic horizon of the pyroclastic rocks unconformably overlying the gneiss complex offered a favorable loci of high grade ore. (3) $N5^{\circ}W$ to $N15^{\circ}$ E-striking faults played an important role in the localization of the orebodies. (4) Conduits of intrusive breccia within the gneiss complex, through which the intrusive breccia intruded into the upper pyroclastic rocks, exist beneath most of the main orebodies. This suggests that the conduits of intrusive breccia served as channelways for the migration of ore fluids.

• 자원환경지질
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• 제25권4호
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• pp.417-433
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• 1992

경북(慶北) 의성(義城)지역 연(鉛)-아연(亞鉛)-동광상(銅鑛床)(전흥(田興), 옥산(玉山) 광산)은 경상분지(慶尙盆地) 백악기(白堊紀) 퇴적암류내의 구조면을 충진한 열수(熱水) 석영-방해석 맥상(脈狀) 광체(鑛體)로 구성된다. 광화(鑛化)작용은 구조적으로 석영-유화물(硫化物)-유염(硫鹽)광물-적철석 정출기, barren 석영-형석 정출기, barren 방해석 정출기 등 3회로 구분된다. 광화(鑛化) I기(期)의 광석(鑛石)광물은 황철석, 황동석, 섬아연석, 방연석 및 Pb-Ag-Bi-Sb계 유염광물(硫鹽鑛物) 등으로서 두 광산의 광물조성은 유사하지만, 유비철석, 자류철석, 테트라헤드라이트, 철을 다량 함유하는(약 21 mole% FeS)섬아연석 등은 옥산(玉山)광산에서만이 산출된다. 변질대 집운모(緝雲母)에 의한 K-Ar 연령은 약 62 Ma로서, 광화(鑛化)작용이 인근 금성산(金城山) 칼데라 화산암류와 도처에 분포하는 산성암맥의 분출 및 관입 활동과 관련된 후기 백악기(白堊紀) 화성활동의 산물이었음을 지시한다. 광화(鑛化) I기(期) 광물정출은 0.7~6.3wt.% NaCl 상당염농도(相當閻濃度)를 갖는 광화유체(鑛化流體)로부터 > $380^{\circ}{\sim}240^{\circ}C$의 온도범위에서 진행되었고, 특히 동(銅)광물은 대부분 > $300^{\circ}C$의 고온에서 침전하였다. 유체포유물(流體包有物) 연구에 의하면, I기 연(鉛)-아연(亞鉛)-동(銅)광물의 침전은 비등(沸騰) 냉각(冷却) 희석(稀釋)등 비교적 복잡한 양식의 광액(鑛液)진화에 기인하였지만, 전흥(田興)광산의 경우 차가운 천수(天水)의 유입(流入)에 따른 냉각(冷却) 및 희석(稀釋)이 우세하였던 반면, 옥산(玉山)광산의 경우는 비등(沸騰)이 우세하게 진행되었다. 광화유체(鑛化流體)의 비등(沸騰)에 근거한 광화(鑛化)작용시의 압력은 초기 약 210 bar에서 후기 약 80 bar에 이르며, 이는 열수계(熱水系)가 정암압(靜岩壓)이 우세한 환경에서 정수압(靜水壓)이 우세한 환경으로 전이되었음을 지시하여 주고 따라서 광화심도(鑛化深度)는 약 900m로 추정된다. 유화물(硫化物)의 유황동위원소(硫黃同位元素) 조성 ($2.9{\sim}9.6$‰)에 근거한 초기 열수유체(熱水流體)의 전(全)유황동위원소값(${\delta}^{34}S_{{\Sigma}S}$)은 약 8.6‰이며, 이는 심부(深部) 화성원(火成源)의 유황이 퇴적암류내 sulfate (?)와 다소 혼합되었음을 나타내는 것으로 사료된다. 한편, 수속 및 산소동위원소 조성은 열수계(熱水系)내의 물이 대부분 천수(天水)로부터 기원하였음을 지시한다. 광물열역학(鑛物熱力學)적 고찰 결과, I기 광화유체(鑛化流體)의 온도 및 유황분압(硫黃分壓)의 변화는 두 광산에서 다소 상이하였다. 즉, 전흥(田興)광산의 경우 온도 감소와 더불어 유황분압(硫黃盆壓)은 황철석-적철석-자철석의 공존선을 따라 지속적으로 감소하였으나, 옥산(玉山)광산의 경우는 초기 황철석-자류철석 공존환경으로부터 후기 황철석-적철석-자철석의 공존환경으로 전이하였다. 한편, 차고 산화(酸化) 상태인 천수(天水)가 광액(鑛液)중에 혼입(混入)됨에 따라 광액의 산소분압(酸素盆壓)은 점차 증가하였다. 동(銅)광물의 침전은 주로 광화유체(鑛化流體)의 냉각에 따른 동염화복합체(銅鹽化複合體)($CuCl^{\circ}$)의 용해도 감소에 기인하였으리라 고려된다. 이러한 냉각 작용은 전흥(田興)광산의 경우 주로 천수혼입(天水混入)에 따른 결과였지만, 옥산(玉山)광산의 경우는 주로 광화유체(鑛化流體)의 비등(沸騰)에 기인하였다.

• 자원환경지질
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• 제25권3호
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• pp.233-243
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• 1992

옥산지역에 위치하는 황학동광상은 초기백악기 퇴적암류내에 발달한 열극을 충진한 열수맥상 광상으로, 구조운동에 수반되어 3회에 걸쳐 생성된 석영 및 방해석맥으로 구성된다. 주된 금속광물로는 황철석, 자류철석, 황동석, 섬아연석, 방연석, 적철석 및 Ag-, Pb-, Bi-sulfosalts로, 이들의 침전은 주로 광화 제 1 기의 0.5~7.6 wt.% NaCl 상당염농도를 갖는 광화유체로부터 $370^{\circ}C$ 에서 약 $200^{\circ}C$ 에 걸쳐 진행되었으며, 광화 작용시의 압력은 <180 bar, 섬도는 700~2,400 m 였다. 광상내에서 보여주는 광물공생관계에 의한 열역학적 고찰과 유체포유물 및 안정동위원소 연구결과 등으로 미루어 본 광상광화유체내 Cu는 주로 chloride complex 상으로 이동되었으며, 주로 광화유체의 냉각작용과 이에 의한 지화학적 환경요인들($fs_2$, $fo_2$, pH)의 변화에 기인하여 침전되었음을 알수 있다. 유황안정동위원소 연구결과, 주광화시기인 광화1기중 광화유체의 ${\delta}^{34}S_{H_2S}$ 값이 초기 8.2‰ 에서 후기 4.7‰ 로 점차 감소함은 광화유체의 비등에 수반되어 수소이온농도와 함께 산소분압이 점진적으로 증가한 결과로 해석되며, 광화유체의 수소 및 산소동위원소 값으로부터 열수계에서 천수가 지배적인 역할을 하였음을 알수 있다.

• Korea-Australia Rheology Journal
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• 제19권4호
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• pp.211-219
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• 2007

Here we demonstrate complex transient behavior of viscoelastic liquid described numerically with the Leonov model in straight and contraction channel flow domains. Finite element and implicit Euler time integration methods are employed for spatial discretization and time marching. In order to stabilize the computational procedure, the tensor-logarithmic formulation of the constitutive equation with SUPG and DEVSS algorithms is implemented. For completeness of numerical formulation, the so called traction boundaries are assigned for flow inlet and outlet boundaries. At the inlet, finite traction force in the flow direction with stress free condition is allocated whereas the traction free boundary is assigned at the outlet. The numerical result has illustrated severe forward-backward fluctuations of overall flow rate in inertial straight channel flow ultimately followed by steady state of forward flow. When the flow reversal occurs, the flow patterns exhibit quite complicated time variation of streamlines. In the inertialess flow, it takes much more time to reach the steady state in the contraction flow than in the straight pipe flow. Even in the inertialess case during startup contraction flow, quite distinctly altering flow patterns with the lapse of time have been observed such as appearing and vanishing of lip vortices, coexistence of multiple vortices at the contraction comer and their merging into one.

• 한국전산유체공학회:학술대회논문집
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• 한국전산유체공학회 1996년도 춘계 학술대회논문집
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• pp.85-92
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• 1996

Numerical simulations are made for the three-dimensional flow around a wing in ground effect craft haying the complex geometry. A numerical tool is developed for the primary design of hull and wing shape of practical Wing-In-Ground effect(WIG) stop. The finite-difference method is utilized to descretize the governing equations and pressure field is obtained by using Marker-And-Cell(MAC) method. The air and water flows are simultaneously simulated in the time-marching solution procedure for the Navier-Stokes equation. The porosity technique and the density function are devised for the implementation of the three-dimensional body-boundary and the free-surface conditions, respectively. In this paper, a craft is modeled simply by three blocks containing a wing mounted on a main body horizontally, with the endplate. The numerical calculations of a WIG advancing in a calm water are performed and the WIG-generated wave profiles are also obtained. In the final paper, details of the numerical methods employed for the present study and calculated results are discussed.

• 대한기계학회논문집
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• 제17권7호
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• pp.1649-1657
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• 1993

This paper reports on a proof-of-concept experimental investigation focused on evaluating the vibration characteristics and control of smart hollow cantilever beams filled with an electro-rheological(ER) fluid. The beams are considered to be of uniform viscoelastic materials and modelled as a viscously-damped harmonic oscillator. Electric field-dependent natural frequencies, loss factors and complex moduli are evaluated and compared among three different beams : two types of different volume fraction of ER fluid and one type of different particle concentration of ER fluid by weight. Modal characteristics of the beams are observed in both the absence and the presence of electric potentials. It is also shown that by constructing active control algorithm the removal of structural resonances and the suppression of tip deflection are obtained. This result provides the feasiblility of ER fluids as an active vibration control element.

• 산업기술연구
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• 제20권A호
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• pp.73-82
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• 2000

This study was implemented to find an optimal model for wastewater treatment processes using PHOENICS(Parabolic, hyperbolic or Elliptic Numerical Integration Code Series) and ASM(Activated Sludge Model). PHOENICS is a general software based upon the laws of physics and chemistry which govern the motion of fluids, the stresses and strains in solids, heat flow, diffusion, and chemical reaction. The wastewater flow and removal efficiency of particle in two phase system of a grit chamber in wastewater treatment plant were analyzed to inquire the predictive aspect of the operational model. ASM was developed for a biokinetic model based upon material balance in complex activated sludge systems, which can demonstrate dynamic and spatial behavior of biological treatment system. This model was applied to aeration tank and settling chamber in Choonchun city, and the modeling result shows dynamic transport in aeration tank. PHOENCS and ASM could be contributed for the optimal operation of wastewater treatment plant.

• 한국전산유체공학회:학술대회논문집
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• 한국전산유체공학회 2009년 추계학술대회논문집
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• pp.201-210
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• 2009

A volume capturing method using unstructured grid system for numerical analysis of multiphase flows is introduced in the present paper. This method uses an interface capturing method (CICSAM) in a volume of fluid(VOF) scheme for phase interface capturing. The novelty of CICSAM lies in the adaptive combination of high resolution discretization scheme which ensures the preservation of the sharpness and shape of the interface while retaining boundedness of the field, and no explicit interface reconstruction which is perceived to be difficult to implement on unstructured grid system. Several typical test cases for multiphase flows are presented, which are simulated by an in-house solution code(PowerCFD). This code employs an unstructured cell-centered method based on a conservative pressure-based finite-volume method with CICSAM. It is found that the present method simulates efficiently and accurately complex free surface flows such as multiphase flows.

• 한국전산유체공학회:학술대회논문집
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• 한국전산유체공학회 2009년 추계학술대회논문집
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• pp.77-83
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• 2009

In this study, we conducted resistance and propulsion performance test of ship composed of the Resistance Test, Propeller Open Water Test and Self Propulsion Test using the CFD(Computational Fluid Dynamics). We used commercial RANS(Reynolds Averaged Navier Stokes equation) solver, as a calculating tool. The unstructured grids were used in a bow and stern of ship, having complex shape, for a convenience of generating grids, and the structured grids were adopted in a central hull and rest of hull having a relatively simple shape which is called hybrid grid method. In addition, The sliding mesh method was adopted to rotate a propeller directly in the Propeller Open Water and Self Propulsion Test. The Resistance Test and Self Propulsion Test were calculated using Volume of Fluid (VOF) model and considering a free surface. And all The three cases were applied realizable k-epsilon model as the turbulence model. The results of calculations were verified for the suitability of calculations by comparing MOERI's EFD results.