• 한국전산유체공학회:학술대회논문집
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• 한국전산유체공학회 2011년 춘계학술대회논문집
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• pp.395-406
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• 2011

In this research a numerical simulation method is developed for moving body in free surface flows using fixed staggered rectangular grid system. The non-linear free surface near the body is defined by marker-density method. The body boundary is defined by line segment connecting the points where the body surface and grid line meet. Continuity equation and Navier-Stokes equations are used as governing equations and the equations are coupled with two-step projection method. The velocities and pressures of body boundary and free surface cells are calculated with simultaneous iterative method. To treat a body movement in a fixed grid system, the volume displaced by moving body is added to the divergence of the body boundary cell. For the verification of the present numerical method. vortex shedding period of advancing cylinder is calculated and the period is compared with existing experiment results. Moreover, added mass and damping coefficients of a vertically excited box are calculated and the computed results are compared with published experiment results. Impulsive pressure and water level variation due to sloshing phenomenon are simulated and the results are compared with published experiment results. Varying the plunger shape, the waves generated by plunging type wave maker are compared with the 2nd order Stokes wave theory The plunger shape generating the wave that shows the best agreement with the theory is represented.

• Bulletin of the Korean Chemical Society
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• 제23권2호
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• pp.295-300
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• 2002

The construction of the T-shaped post-column flow cell has been changed to enhance the practicability as a UV-visible absorbance detector for capillary electrophoresis. In this new design, a rectangular cube-shaped inner structure is employed, which completely fits the outer rectangular tubing. This arrangement has greatly facilitated the fabrication of the T-cells. In addition, the volume for the auxiliary flow has been dramatically reduced down to 300 ${\mu}L$, and its volume flow rate is optimized at 4.2 ${\mu}L$/min. The short optical path length in the sheath flows (500 ${\mu}m$ on each side) minimizes background absorption, and thus enhances its performance in low-UV wavelengths. We have optimized the auxiliary flow rate at 50 ${\mu}m$/s, so that migration times are insensitive to the flow rate. This optimization has improved repeatabilities in migration times and peak heights. A double-beam detection scheme using a pair of photodiodes is employed to increase the signal-to-noise ratio.

• Advances in aircraft and spacecraft science
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• 제6권6호
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• pp.515-528
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• 2019

The structural vibrations of a flat plate induced by fluctuating wall pressures within wall-bounded transonic jet flow downstream of a high-aspect ratio rectangular nozzle are simulated. The wall pressures are calculated using Hybrid RANS/LES CFD, where LES models the large-scale turbulence in the shear layers downstream of the nozzle. The structural vibrations are computed using modes from a finite element model and a time-domain forced response calculation methodology. At low flow speeds, the convecting turbulence in the shear layers loads the plate in a manner similar to that of turbulent boundary layer flow. However, at high nozzle pressure ratio discharge conditions the flow over the panel becomes transonic, and the shear layer turbulence scatters from shock cells just downstream of the nozzle, generating backward traveling low frequency surface pressure loads that also drive the plate. The structural mode shapes and subsonic and transonic surface pressure fields are transformed to wavenumber space to better understand the nature of the loading distributions and individual modal responses. Modes with wavenumber distributions which align well with those of the pressure field respond strongly. Negative wavenumber loading components are clearly visible in the transforms of the supersonic flow wall pressures near the nozzle, indicating backward propagating pressure fields. In those cases the modal joint acceptances include significant contributions from negative wavenumber terms.

• 한국군사과학기술학회지
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• 제21권2호
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• pp.225-234
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• 2018

In this paper, we consider a problem of partitioning a search area into smaller rectangular regions, so that multiple platforms can conduct search operations independently without requiring unnecessary coordination among themselves. The search area consists of cells where each cell has some prior information regarding the probability of target existence. The detection probability in particular cell is evaluated by multiplying the observation probability of the platform and the target existence probability in that cell. The total detection probability within the search area is defined as the cumulative detection probability for each cell. However, since this search area partitioning problem is NP-Hard, we decompose the problem into three sequential phases to solve this computationally intractable problem. Additionally, we discuss a special case of this problem, which can provide an optimal analytic solution. We also examine the performance of the proposed approach by comparing our results with the optimal analytic solution.

• International Journal of Aeronautical and Space Sciences
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• 제3권1호
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• pp.95-104
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• 2002

Numerical solution of the full Navier-Stokes equation as well as the energy equation has been obtained for the unsteady natural convection in a rectangular enclosure. One side wall was maintained at very high temperature simulating fires. Especially the effect of surface radiation was taken into account. While the enclosed air was assumed to be transparent, the internal walls directly interacted one another through the surface radiation. Due to a significant temperature difference in the flow field, the equation of state was used instead of the Boussinesq approximation. It was found that the rapid heating of the adiabatic ceiling and floor by the incoming radiation from the hot wall made the evolution at thermo-fluid field highly unstable in the initial period. Therefore, the secondary cells brought about at the floor region greatly affected the heat transfer mechanism inside the enclosure. The heat transfer rate was augmented by the radiation, resulting in requiring less time for the flow to reach the steady state. At the steady state neglecting radiation two internal hydraulic jumps were clearly observed in upper/left as well as in lower/right comer. However, the hydraulic jump in the lower/right comer could not be observed for the case including radiation due to its high momentum flow over the bottom wall. Radiation resulted in a faster establishment of the steady state phenomena.

• 대한기계학회논문집A
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• 제28권8호
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• pp.1183-1189
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• 2004

A novel cell count method, which can improve the count efficiency and reduce contamination problem, was presented using micro lattice engraved on culture dish. The micro lattice has feature of $50{\mu}m{\times}50{\mu}m$ rectangular shape, $2{\mu}m$ line width, and $2{\mu}m$ depth in $3mm{\times}3mm$ area. In this paper, nickel mold was fabricated with thickness of 3mm and diameter of 80 mm, and transcription of the micro lattice on a polystyrene cell culture dish was performed by hot embossing at $200\;^{\circ}C$. The tedious and error-prone harvest/load processes of conventional cell counts with a hemocytometer could be omitted, and these advantages became magnified during periodical counts involving long-term cultures. SupT1 cells and HeLa cells were cultivated with the dish for 7 days in $CO_2$ incubator and counted as $371.84/mm^2$ and $123.36/mm^2$, respectively, during the cultivation without harmful effects on the cells.

• 대한본초학회지
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• 제21권4호
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• pp.183-187
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• 2006

Objectives : Southern, northern, and wild types of Osterici Radix, and Notopterigii Rhizoma et Radix imported from China are circulated in Korea. Morphological identification was attempted by comparing powder forms of these materials. Methods : To make the specimen, the samples were grinded, and the powder was mounted by a solution of Glycerin, Acetic acid and Water at the rate of 1 : 1 : 1. The specimen was mounted by optic microscope, photographs were taken and the characteristics were sketched in lines. Result : 1. Korean Osterici Radix was yellow-brown, but Chinese Notopterigii Rhizoma et Radix was dark-brown. 2. Oil ducts were mostly broken, and most of secretory cells were narrow and long, including yellow or light yellow secretion and starch grain. 3. Parenchyma cells were rectangular, and southern type of Osterici Radix and Chinese Notopterigii Rhizoma et Radix include lots of starch grain in parenchyma cells, while northern type of Osterici Radix and wild Osterici Radix include a little. 4. Vessels were usually reticulate vessel, and the diameter of the vessels of Korean Osterici Radix was $25{\sim}88{\mu}m$, while that of the vessels of Chinese Notopterigii Rhizoma et Radix was $13{\sim}52{\mu}m$. 5. The surface of accessory cells were light brown with the shape of irregular polygon. Conclusion : Southern type of Osterici Radix, nothern type of Osterici Radix, wild Osterici Radix, and Chinese Notopterigii Rhizoma et Radix were all alike, except the amount of starch grain in parenchyma cells.

• 대한전자공학회논문지TC
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• 제45권8호
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• pp.60-68
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• 2008

구형 도파관 기법을 이용하여 다양한 모양을 가진 주기적인 metamaterial (MTM) 셀의 복소 유전율과 투자율을 시뮬레이션으로 추출하였다. 이 도파관은 PEC 벽과 PMC 벽으로 구성된 가상적인 것이고, 고려된 MTM 셀의 모양은 thin wire (TW), single split-ring resonator (SSRR), double SRR (DSRR), modified SRR, 그리고 TW와 DSRR이 결합된 구조이다. TW는 음의 유전율/양의 투자율, SRR은 양의 유전율/음의 투자율, 그리고 TW와 DSRR을 합친 구조는 유전율과 투자율이 동시에 음이 되는 영역이 나타남을 확인하였다. 각 셀의 파라미터에 따른 유전율과 투자율의 변화를 살펴보았다. 추가적인 연구로서 상기 도파관 기법의 단점을 보완하는 시 영역 신호를 이용한 추출 방법을 소개했다.

• 대한의용생체공학회:의공학회지
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• 제43권1호
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• pp.1-10
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• 2022

Non-alcoholic fatty liver disease(NAFLD) is excessive hepatic lipid accumulation mainly caused by obesity. This study aimed to evaluate whether micro-current stimulation(MCS) could modulate lipid metabolism regarding the Sirt1/AMPK pathway, fatty acid β-oxidation pathway, and lipolysis and lipogenesis-related factors in FL83B cells. For the NAFLD cell model, FL83B cells were treated with oleic acid for lipid accumulation. MCS were stimulated for 1 hr and used frequency 10 Hz, duty cycle 50%, and biphasic rectangular current pulse. The intensity of MCS was divided into 50, 100, 200, and 400 ㎂. Through the results of Oil red O staining, it was confirmed that MCSs with the intensity of 200 ㎂ and 400 ㎂ significantly reduced the degree of lipid droplet formation. Thus, these MCS intensities were applied to western blot analysis. Western blot analysis was performed to analyze the effects of MCS on lipid metabolism. MCS with the intensity of 400 ㎂ showed that significantly activated the Sirt1/AMPK pathway, a key pathway for regulating lipid metabolism in hepatocytes, and fatty acid β-oxidation-related transcription factors. Moreover, it activated the lipolysis pathway and suppressed lipogenesis-related transcription factors such as SREBP-1c, FAS, and PPARγ. In the case of MCS with the intensity of 200 ㎂, only PGC1α and SREBP-1c showed significant differences compared to cells treated only with oleic acid. Taken together, these results suggested that MCS with the intensity of 400 ㎂ could alleviate hepatic lipid accumulation by modulating lipid metabolism in hepatocytes.

• 한국산림과학회지
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• 제65권1호
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• pp.74-79
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• 1984

우리나라산(産) 버드나무류(類) 중(中) 사시나무속(屬) 6 수종(樹種), 버드나무속(屬) 5 수종(樹種)을 선택(選澤)하여 간재(幹材)의 대질부(木質部) 조직특성중(組織特性中) 방사조직(放射組織)에 대(對)한 해부학적(解剖學的) 식별(識別)에 관(關)하여 조사(調査)한 결과(結果)를 요약(要約)하면 다음과 같다. 방사조직(放射組織)의 형(型)은 사시나무속(屬)은 단열동성(單列同性)이고, 버드나무속(屬)은 단열이성(單列異性)이었다. 버드나무속(屬)의 단열이성방사조직(單列異性放射組織) 중(中) 직립세포(直立細胞)를 장방형(長方型)과 정방형(正方型)으로 세분(細分)했다. 평복세포(平伏細胞) 방사조직장(放射組織長)은 사시나무속(屬)이 최소(最少) 및 최대치(最大値)가 $26.84{\sim}212.28{\mu}$, 버드나무속(屬)이 $46.36{\sim}170.80{\mu}$의 범위(範圍)였고, 또 버드나무속(屬)의 직립세포(直立細胞)에 있어서 장방형(長方型)은 $26.84{\sim}70.76{\mu}$, 정방형(正方型)은 $17.08{\sim}43.92{\mu}$ 범위(範圍)였다. 평복세포(平伏細胞)의 방사조직폭(放射組織幅)은 사시나무속(屬)이 최소(最少) 및 최대치(最大値)가 $12.20{\sim}24.40{\mu}$, 버드나무속(屬)이 $12.20{\sim}26.84{\mu}$의 범위(範圍)였고, 또 버드나무속(屬)의 직립세포(直立細胞)에 있어서 장방형(長方型)은 $9.76{\sim}41.48{\mu}$, 정방형(正方型)은 $19.52{\sim}46.36{\mu}$ 범위(範圍)였다. 촉단면상(觸斷面上)에서 방사조직(放射組織)의 고(高)는 사시나무속(屬)이 $65.88{\sim}414.80{\mu}$, 버드나무속(屬)이 $65.88{\sim}439.20{\mu}$의 범위(範圍)이였다. 방사조직(放射組織)의 폭(幅)은 사시나무속(屬)이 $4.88{\sim}24.40{\mu}$, 버드나무속(屬)이 $7.32{\sim}21.96{\mu}$의 범위(範圍)였었다. 촉단면상(觸斷面上)에서의 방사조직(放射組織)의 수(數)(세포고(細胞高))는 사시나무속(屬)이 3~26 세포고(細胞高)이고 버드나무속(屬)이 2~21 세포고(細胞高)이었다.