• 대한조선학회논문집
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• 제54권6호
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• pp.492-500
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• 2017

In the study, numerical simulation on the greenwater impact load of free surface offshore structure in the regular waves using fixed cartesian grid system and Modified Marker-Density (MMD) method were carried out and the results were reviewed. In order to compare numerical simulation and experimental results, the FPSO with the scale ratio of 1/100 model ship with fixed rectangular deck was selected and turbulence characteristic of the flow was considered by applying the Sub-Grid Scale (SGS) in laminar flow. As a result, it is reviewed how the greenwater impact load inflowed from bow in regular headsea wave influence the flow on the deck and the flow characteristic by numerical simulation and the experiment results were compared and reviewed. Based on this study, it would be useful to numerically study the effect of greenwater on offshore structure.

• 대한조선학회논문집
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• 제51권5호
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• pp.419-428
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• 2014

This paper presents a numerical simulation method for the flow around advancing ships in regular waves by using a rectilinear grid system. Because the grid lines do not consist with body surface in the rectilinear grid system, the body geometries are defined by the interaction points of those grid lines and the body surface. For the satisfaction of body boundary conditions, no-slip and divergence free conditions are imposed on the body surface and body boundary cells, respectively. Meanwhile, free surface is defined with the modified marker density method. The pressure on the free surface is determined to make the pressure gradient terms of the governing equations continuous, and the velocity around the free surface is calculated with the pressure on the free surface. To validate the present numerical method, a vortex induced vibration (VIV) phenomenon and flows around an advancing Wigley III ship model in various regular waves are simulated, and the results are compared with existing and corresponding research data. Also, to check the applicability to practical ship model, flows around KRISO Container Ship (KCS) model advancing in calm water are numerically simulated. On the simulations, the trim and the sinkage are set free to compare the running attitude with some other experimental data. Moreover, flows around the KCS model in regular waves are also simulated.

• 대한조선학회지
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• 제25권4호
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• pp.13-27
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• 1988

TUMMAC차분법(差分法)이 두 가지의 삼차원파(三次元波), 즉 배의 항주(航走)에 따른 파형(波形)과 수직사각주(垂直四角柱) 주위의 쇄파해석(碎波解析)에 적용(適用)되어졌다. Series 60($C_B=0.6$) 모형선(模型船)과 HSVA 모형선(模型船)의 선수부(船首部)에 의한 파형(波形)이 자유표면(自由表面)과 선체후반부(船體後半部)에서의 boundary cell 처리를 엄밀화한 $TUMMAC-IV_{vm1}$방법(方法)에 의하여 계산(計算)되어졌으며, 그 결과가 실제(實際)의 실험결과(實驗結果)들과 비교(比較)되었다. 실험결과(實驗結果)와의 비교를 통하여, $TUMMAC-IV_{vm1}$방법(方法)은 배에 의한 비선형파(非線形波)의 특성해석(特性解析)에 매우 응용성(應用性)이 높음을 보였다. 특히, 비대선형(肥大船型)인 HSVA 모형선(模型船)의 경우는 계산(計算)된 비선형선수파(非線形船首波)의 특성(特性)이 실험결과(實驗結果)와 좋은 일치를 보였다. 수직사각주(垂直四角柱)주위의 쇄파(碎波)를 포함한 심한 비선형파(非線形波)가 삼차원비선형파(三次元非線形波)의 대표적(對表的)인 예(例)로써 TUMMAC-VI 방법(方法)에 의하여 계산(計算)되었다. TUMMAC-VI 방법(方法)은 이층류(二層流)를 함께 푸는 방법(方法)으로, 두가지 유체(流體) 사이의 밀도변화(密度變化), 즉 marker-density를 이용하여 interface를 결정하게 된다. 그러나, 비압축성유체(非壓縮性流體)에 관한 N-S 방정식(方程式)의 해(解)이므로, 그 밖의 계산(計算)에서는 각각의 대표적(對表的)인 밀도(密度)를 사용한다. 계산결과(計算結果)는 삭가주(四角柱) 앞부분의 원형파(圓形波)와 앞어깨에서의 심한 경사를 가지는 파(波), 뒷부분에서의 복잡(複雜)한 쇄파현상(碎波現像)들이 실제의 파특성(波特性)을 잘 나타내어 주었다. TUMMAC-VI 방법(方法)은 interface의 처리를 포함하여 앞으로도 개선(改善)의 여지가 많으며, 단지 공기(空氣)와 물만이 아닌 일반적(一般的)인 이층류(二層流)의 해석에도 폭 넓게 이용될 수 있으리라 본다.

• 대한임상검사과학회지
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• 제44권3호
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• pp.103-111
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• 2012

Low-Density Lipoprotein cholesterol (LDLC) is the most important marker for the treatment of hyperlipidemia in NCEP-ATP III(National Cholesterol Education Program-Adult Treatment Panel III) guideline. Therefore, LDL cholesterol is pathologically meaningful, accurate measurement should be a top priority. Currently, LDLC is directly measured in most cases, but, the estimate is still used in mass health examination or screening test. This study is about the comparison of LDL-Cholesterol direct measurement with the estimate using various formula (Friedewald: [LDL-F=TC-HDL-TG/5], Nakajima: [LDL-N=TC-HDL-TG/4], Hattori: [LDL-H =0.94TC-0.94HDL-0.19TG], Puavilai: [LDL-P=TC-HDL-TG/6], Carvalho: [LDL-C=3(TC-HDL)/4]) for calculating more accurate value. We analyzed total cholesterol (TC), try-glyceride (TG), high-density lipoprotein cholesterol (HDLC), and LDLC levels of 210 subjects between June and November in 2011. Until now, the Friedewald formula is the most commonly used estimate for the LDLC. When Friedewald formula was applied, the correlation coefficient (r) was 0.940, showing high correlation. But, the result of the direct method was significantly different, compared with those of the Friedewald formula in triglyceride levels ${\geq}400mg/dL$(p<0.05). There was the highest correlation when we used LDL-P formula(r=0.947) in triglyceride levels <400 mg/dl. Also there was the lowest mean difference regardless of triglyceride level. Therefore, the study showed that TG/6 is more precise means of calculation than TG/5. On the other hand, the calculation of LDL-Cholesterol was underestimated, compared with direct measurement. It is necessary to have more data and modified Friedewald formula should be used for the accurate calculation.