• 한국컴퓨터정보학회논문지
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• 제27권4호
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• pp.79-88
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• 2022

본 연구는 20대 비만 여성에게 적합한 보디스 원형 개발을 위해 프랑스, 일본 패션교육기관의 원형과 우리나라 교육용 원형 1개, 우리나라 산업체용 원형 2개 등 총 5개 패턴 제도법을 비교·분석하였다. 이를 통해 플러스 사이즈 여성 의복 개발에 적합한 보디스 원형 패턴 제도법을 알아보고자 하였다. 패턴제도를 위해 패턴1은 앞품, 뒤품, 젖가슴둘레, 목둘레, 등길이 등 가장 많은 신체치수를 적용하였고, 패턴2, 패턴4, 패턴5는 젖가슴둘레, 등길이를 기준으로 모든 패턴을 제작하였다. 외관평가 결과, 패턴3이 앞중심길이의 적합성, 옆허리둘레선 위치의 적합성 항목을 제외하고 모든 항목에서 가장 우수한 패턴으로 평가되었다. 그러나 옆선의 수직, 옆허리둘레선 위치의 적합성, 뒤진동둘레 위치 및 형태의 적합성, 뒤어깨다트 위치의 적합성 등의 항목에서는 부적합한 것으로 평가되었다. 보디스 원형은 젖가슴둘레 치수를 기준으로 대부분의 패턴 제도가 이루어지나 비만 여성의 경우 목둘레 설정, 어깨길이 설정에 있어서는 다른 제도법이 필요할 것으로 생각된다. 또, 복부 돌출로 앞중심길이 설정 방법에 대한 개발도 요구되었다.

• 한국분말야금학회:학술대회논문집
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• 한국분말야금학회 2000년도 춘계학술강연 및 발표대회 강연 및 발표논문 초록집
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• pp.9-10
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• 2000

An important business-field of world-wide steel-industry is the coating of thin metal-sheets with zinc, zinc-aluminum and aluminum based materials. These products mostly go into automotive industry. in particular for the car-body. into building and construction industry as well as household appliances. Due to mass-production, the processing is done in large continuously operating plants where the mostly cold-rolled metal-strip as the substrate is handled in coils up to 40 tons unwind before and rolled up again after passing the processing plant which includes cleaning, annealing, hot-dip galvanizing / aluminizing and chemical treatment. In the liquid Zn, Zn-AI, AI-Zn and AI-Si bathes a combined action of corrosion and wear under high temperature and high stress onto the transfer components (rolls) accounts for major economic losses. Most critical here are the bearing systems of these rolls operating in the liquid system. Rolls in liquid system can not be avoided as they are needed to transfer the steel-strip into and out of the crucible. Since several years, ceramic roller bearings are tested here [1.2], however, in particular due to uncontrollable Slag-impurities within the hot bath [3], slide bearings are still expected to be of a higher potential [4]. The today's state of the art is the application of slide bearings based on Stellite\ulcorneragainst Stellite which is in general a 50-60 wt% Co-matrix with incorporated Cr- and W-carbides and other composites. Indeed Stellite is used as the bearing-material as of it's chemical properties (does not go into solution), the physical properties in particular with poor lubricating properties are not satisfying at all. To increase the Sliding behavior in the bearing system, about 0.15-0.2 wt% of lead has been added into the hot-bath in the past. Due to environmental regulations. this had to be reduced dramatically_ This together with the heavily increasing production rates expressed by increased velocity of the substrate-steel-band up to 200 m/min and increased tractate power up to 10 tons in modern plants. leads to life times of the bearings of a few up to several days only. To improve this situation. the Mechanical Alloying (MA) TeChnique [5.6.7.8] is used to prOduce advanced Stellite-based bearing materials. A lubricating phase is introduced into Stellite-powder-material by MA, the composite-powder-particles are coated by High Energy Milling (HEM) in order to produce bearing-bushes of approximately 12 kg by Sintering, Liquid Phase Sintering (LPS) and Hot Isostatic Pressing (HIP). The chemical and physical behavior of samples as well as the bearing systems in the hot galvanizing / aluminizing plant are discussed. DependenCies like lubricant material and composite, LPS-binder and composite, particle shape and PM-route with respect to achievable density. (temperature--) shock-reSistibility and corrosive-wear behavior will be described. The materials are characterized by particle size analysis (laser diffraction), scanning electron microscopy and X-ray diffraction. corrosive-wear behavior is determined using a special cylinder-in-bush apparatus (CIBA) as well as field-test in real production condition. Part I of this work describes the initial testing phase where different sample materials are produced, characterized, consolidated and tested in the CIBA under a common AI-Zn-system. The results are discussed and the material-system for the large components to be produced for the field test in real production condition is decided. Outlook: Part II of this work will describe the field test in a hot-dip-galvanizing/aluminizing plant of the mechanically alloyed bearing bushes under aluminum-rich liquid metal. Alter testing, the bushes will be characterized and obtained results with respect to wear. expected lifetime, surface roughness and infiltration will be discussed. Part III of this project will describe a second initial testing phase where the won results of part 1+11 will be transferred to the AI-Si system. Part IV of this project will describe the field test in a hot-dip-aluminizing plant of the mechanically alloyed bearing bushes under aluminum liquid metal. After testing. the bushes will be characterized and obtained results with respect to wear. expected lifetime, surface roughness and infiltration will be discussed.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2015년도 제49회 하계 정기학술대회 초록집
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• pp.188.1-188.1
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• 2015

For present investigation Fe/MgO/Fe/Co multilayer stack is grown on Si substrate using e-beam evaporation in ultrahigh vacuum. This stack is irradiated perpendicularly by 120 MeV $Ag^{8+}$ at different fluences ranging from $1{\times}10^{11}$ to $1{\times}10^{13}ions/cm^2$ in high vacuum using 15UD Pelletron Accelerator at Inter University Accelerator Centre, New Delhi. Magnetic measurements carried out on pre and post irradiated stacks show significant changes in the shape of perpendicular hysteresis which is relevant with previous observation of re-orientation of magnetic moment along the direction of ion trajectory. However increase in plane squareness may be due to the modification of interface structure of stacks. X-ray reflectivity measurements show onset of interface roughness and interface mixing. X-ray diffraction measurements carried out using synchrotron radiation shows amorphous nature of MgO and Co layer in the stack. Peak corresponding body centered Fe [JCPDS-06-0696] is observed in X-ray diffraction pattern of pre and post irradiated stacks. Peak broadening shows granular nature of Fe layer. Estimated crystallite size is $22{\pm}1nm$ for pre-irradiated stack. Crystallite size first increases with irradiation then decreases. Structural quality of these stacks was further studied using transmission electron microscopic measurements. Thickness from these measurements are 54, 36, 23, 58 and 3 nm respectively for MgO, Fe, MgO, Fe+Co and Au layers in the stack. These measurements envisage poor crystallinity of different layers. Interfaces are not clear which indicate mixing at interface. With increase fluence mixing and diffusion was increased in the stack. X-ray absorption spectroscopic measurements carried out on these stacks show changes of Fe valence state after irradiation along with change of O(2p)-metal (3d) hybridized state. Valence state change predicts oxide formation at interface which causes enhanced in-plane magnetization.

• 한국포장학회지
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• 제21권3호
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• pp.97-106
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• 2015

RTE(ready-to-eat)형 전자레인지 가열용 제품들의 가열 조리 시 특정 부위의 열 변형이 발생하여 전자레인지 포장재의 재질 및 형태별 가열 패턴을 조사하였다. 국내에서 유통되고 있는 시료 9종 중 5개의 시료에서 열 변형이 발생되었고, 국외에서 유통되고 있는 시료 11종 중 8종에서 열 변형이 발생되었다. 국외 시료의 경우 국내 시료보다 열 변형 정도는 덜 하였지만 일부 발생되는 것을 확인하였다. 또한 트레이 타입 용기에 열 변형이 발생하는 소스를 담고 전자레인지로 가열하였을 때도 리드지 및 컵에서 열 변형이 관찰되었다. 국내외에서 유통되고 있는 전자레인지 가열용 제품의 염도, 당도, pH 및 점도를 측정한 결과 열 변형 발생 유무 및 정도에 따른 일정한 경향은 없었다. 하지만 극히 낮거나 높은 점도를 가진 시료에서 열 변형이 나타나지 않았고 내용물의 형태 및 포장재의 형태에 따라 열 변형의 차이가 있었다. 따라서 제품의 열 전환 및 열전달을 고려하여 포장재의 깊이 등 설계를 반영하여 포장 내 전자파의 집중을 방지하는 등의 기술 도입이 필요할 것으로 판단된다.

• 수산해양기술연구
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• 제22권4호
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• pp.61-70
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• 1986

In accordance with a rapid growth of demani on aquatic animals, researches of the unused fishery resources On the deep sea b~d in the Korean Waters has been and will be required. The authors carried out a series of fishing experiments to investigate the available resources and to find the effective fishing method on the deep sea bed of the Korean East Sea. In the experiments, 19 kinds of traps which are different from each other in shape, mesh size and entrance diameter were used. The fishing experiments w~r;; carried out in four areas of 20Dm, 600.'11, 800m and 1000.'11 deep respectively, by the Pusan 402 (30:) GT) and the Pusan 403 (279GT), the training ships of National Fisheries University of Pusan, during August, 1986. The catc~ were analyzed with the size, the depth and the construction of traps. The results obtained can be summarized as follows: 1. Main species of the catch w~re pink shrimp, Pandalus bolelis, a kind of welks, Buccimum striatissimum and a kind of larg~ crabs. Chiono8cetes japonicus and the another species were few. 2. The CPUE value (expressed by the number of catch per trap in this paper) of pink shrimp was the highest in the depth of 20J-n around, and the value in the depth of 600.'11 or more decreased gradually with an increase of the depth. But, the value of Buccimum straitissimum was much higher in the depth of 6:J:)!1I or more than that in the depth of 200m around. On the other hand, the value of Chion:Jecetes japonjcus was very low in general. 3. The iniividual body size of the catch differed with the depth. Pink shrimps caught in the depth of 200m around were smaller than those in the depth of 600.'11 or more. In contrast with this, Baccimum striatissim:t.m caught in the depth of 200m around were larger than those in the depth of 600.'11 or more. 4. Depending on the selection curve in Ishida's method for the mesh size of trap webbing, the carapace length of pink shrimp and the shell length of Buccimum striatissimum which are equivalent to 100% relative catching efficiency can be estimated about 3.5cm and 6.5cm or so respectively. 5. The number of catch of pink shrimp and Buccimum striatissimum by the 60.'1'1.'11 entrance diameter of trap were less than that by the 90mm, 120mm and 150mm, even thogh the diffierence am~r, g 9:Jmm, 120.'11.'11 and 150:1'.'11 are not so large.

• 한국임상수의학회지
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• 제28권5호
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• pp.510-515
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• 2011

개에서 컴퓨터단층촬영술을 이용하여, 촬영 자세에 따른 정상 폐의 용적과 밀도를 정량적으로 평가하였다. 각각 6 마리의 페키니즈견과 말티즈견에서 컴퓨터단층촬영을 실시하면서 자세를 앙와위, 좌측과 우측 횡와위, 그리고 흉와위로 변경하였다. 컴퓨터단층촬영을 실시하는 동안 일정한 정도의 양압환기를 실시하였다. 폐용적과 밀도는 CT 영상의 삼차원 재구성 방식을 통해 측정하였고, 전체 폐용적 및 밀도, 좌측과 우측 폐의 용적과 밀도를 각각 측정하였다. 삼차원 재구성 결과 폐의 모양은 두 품종견에서 매우 다르게 나타났다. 폐용적과 밀도는 촬영 자세를 변경하는 동안 두 품종견에서 모두 유의적인 변화를 보이지 않았다. 오른쪽 폐용적이 왼쪽 폐에 비해 유의적으로 약 $66.91{\pm}25.1$ ml 만큼 컸다. 페키니즈 견과 말티즈 견의 체중 차이가 유의적이었으며, 체중과 흉와위로 촬영한 폐용적 간에 선형관계가 관찰되었다. 좌우측 횡와위 촬영에서 중력의 영향을 받는 쪽의 폐는 반대쪽 폐에 비해 밀도는 높고 용적은 감소되었다. 컴퓨터단층촬영으로 측정한 전체 폐용적은 폐밀도와 관련이 있었으며, 폐밀도가 정상 폐용적을 유추하는데 유용하게 사용될 것으로 생각된다.

• 대한치과보철학회지
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• 제53권2호
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• pp.120-127
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• 2015

목적: 4종의 임플란트 나사산이 골유착 중간과정과 완료 이후 단계에서 보이는 응력분산 특성을 평가하고자 한다. 재료 및 방법: 실린더형 몸체(외경 4.1 mm 길이 10 mm)에 이전연구에서 식립 특성이 우수하게 평가되었던 V-자형 나사산과 다른 3종(buttress형, reverse buttress형, square형)의 나사산을 가진 4종의 임플란트가 악골에 매식된 복합체 모델을 CAD 프로그램으로 제작하였다. 지대주 상부에 100 N의 힘을 임플란트 장축과 30도 방향으로 부하하고 인접골 응력분포를 유한요소 해석하였다. 응력분산 특성이 골유착 진척 상태에 따라 달라질 수 있다는 가정하에 임플란트/골 계면을 골유착 미숙단계와 골유착 완료단계의 두 가지로 구분하여 분석하였다. 골유착 미숙단계는 임플란트/골 계면을 비선형 contact 조건(마찰계수 0.3)으로 모사하였고, 골유착이 완료된 단계에 대해서는 계면이 충분히 결합된 것으로 간주하여 접합(bonding) 조건을 부여하였다. 결과: 골유착 정도에 따라 임플란트의 응력분산 특성이 달라졌다. 골유착 미숙단계에서는 골응력과 나사산에 따른 응력 특성의 차이도 상대적으로 컸고 골유착 완료단계에서는 골응력의 절대값과 나사산간 차이가 모두 감소하였으며, V-자형 나사산의 응력분산 특성은 골유착 미숙 및 완료단계에서 모두 4종 나사산의 중간 정도였다. 이로부터 나사산 디자인의 차이는 임플란트 식립후 골유착이 진행되는 과정까지 영향을 미치며, 일단 골유착이 완료되면 나사산의 영향은 급격히 감소할 것임을 추론할 수 있었다. 결론: V-자형 나사산의 응력분산 특성은 골유착이 이루어지는 단계와 완료된 이후 단계 전기간 동안 4종 나사산의 중간 정도였다.

• 사상체질의학회지
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• 제8권1호
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• pp.101-186
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• 1996

1. 연구배경 : 사상의학의 가장 중요한 요점은 체질진단이다. 그간 다양한 체질변증에 관한 연구가 있었지만 신체 각부의 형태학적인 연구, 특히 얼굴을 대상으로 한 연구는 거의 전무하였다. 저자들은 그 동안 전일적이고 직관적으로 표현된 동의수세보원의 형태적 묘사를 정량화하여 정리하고, 이 자료를 체질진단의 근거자료로 삼고자 하는 연구의 일환으로 먼저 두안부(頭顔部)의 형태를 태음인 소음인 소양인 별로 그 형상적 특징을 찾아내고자 하였다. 2. 방법 : 1995년 7월부터 1995년 12월까지 경희의료원 부속한방병원 외래환자 및 직원을 대상으로 설문지 및 임상적 치료 경과를 통하여 체질적 경향성이 뚜렷한 대상자를 선별하고 동일촬영 조건을 통하여 얻은 얼굴 사진 중 형태특이자를 제외한 170례의 고경(전두고외 26항목) 방사경(두최대장외 22항목) 및 폭경(안최대폭외 18항목)등 총 69항목을 측정한 후 이를 분석하여 체질별 상이점을 도출하였다. 3. 결과 : 체질별 두면부의 형태학적인 특징을 수치화하여 설명할 수 있게 되었고, 나아가 직관적이고 전일적인 형태를 구체화시킬 수 있는 특징을 도출할 수 있었다. 4. 결론 : 이상의 결과를 이용하여 체질별 각 부분의 형태를 계량화하여 비교 설명하고, 이를 이용하여 체질판별공식을 만들었다.

• 한국표면공학회:학술대회논문집
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• 한국표면공학회 1999년도 추계학술발표회 초록집
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• pp.15-15
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• 1999

In chip plating, several parameters must be taken into consideration. Current density, solution concentration, pH, solution temperature, components volume, chip and media ratio, barrel geometrical shape were most likely found to have an effect to the process yields. The 3 types of barrels utilized in chip plating industry are the conventional rotating barrel. vibrational barrel (vibarrel), and the centrifugal type. Conventional rotating barrel is a close type and is commonly used. The components inside the barrel are circulated by the barrel's rotation at a horizontal axis. Process yield has known to have higher thickness deviation. The vibrational barrel is an open type which offers a wide exposure to electrolyte resulting to a stable thickness deviation. It rotates in a vertical axis coupled with multi-vibration action to facilitate mixed up and easy transportation of components, The centrifugal barrel has its plated work centrifugally compacted against the cathode ring for superior electrical contact with simultaneous rotary motion. This experiment has determined the effect of barrel vibration intensity to the plating thickness distribution. The procedures carried out in the experiment involved the overall plating process., cleaning, rinse, Nickel plating, Tin-Lead plating. Plating time was adjusted to meet the required specification. All other parameters were maintained constant. Two trials were performed to confirm the consistency of the result. The thickness data of the experiment conducted showed that the average mean value obtained from higher vibrational intensity is nearer to the standard mean. The distribution curve shown has a narrower specification limits and it has a reduced variation around the target value, Generally, intensity control in vi-barrel facilitates mixed up and easy transportation of components, However, it is desirable to maintain an optimum vibration intensity to prevent solution intrusion into the chips' internal electrode. A cathodic reaction can occur in the interface of the external and internal electrode. $2HD{\;}+{\;}e{\;}{\rightarrow}20H{\;}+{\;}H_2$ Hydrogen can penetrate into the body and create pressure which can cause cracks. At high intensity, the chip's motion becomes stronger, its contact between each other is delayed and so plating action is being controlled. However, the strong impact created by its collision can damage the external electrode's structure thereby resulting to bad plating condition. 1 lot of chip was divided into two equal partion. Each portion was loaded to the same barrel one after the other. Nickel plating and tin-lead plating was performed in the same station. Portion A maintained the normal barrel vibration intensity and portion B vibration intensity was increased two steps higher. All other parameters, current, solution condition were maintained constant. Generally, plating method find procedures were carried out in a best way to maintained the best plating condition. After plating, samples were taken out from each portion. molded and polished. Plating thickness was investigated for both. To check consistency of results. 2nd trial was done now using different lot of another characteristics.

• Wind and Structures
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• 제7권5호
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• pp.317-332
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• 2004

Wind tunnel experiments were conducted under highly turbulent and disturbed flow conditions over a solid/perforated plate with a long splitter plate in its plane of symmetry. The effect of varied level of perforation of the normal plate on fluctuating velocities and fluctuating pressures measured across and along the separation bubble was studied. The different perforation levels of the normal plate; that is 0%, 10%, 20%, 30%, 40% and 50% are studied. The Reynolds number based on step height was varied from $4{\times}10^3$ to $1.2{\times}10^4$. The shape and size of the bubble vary with different perforation level of the normal plate that is to say the bubble is reduced both in height and length up to 30% perforation level. For higher perforation of the normal plate, bubble is completely swept out. The peak turbulence value occurs around 0.7 to 0.8 times the reattachment length. The turbulence intensity values are highest for the case of solid normal plate (bleed air is absent) and are lowest for the case of 50% perforation of the normal plate (bleed air is maximum in the present study). From the analysis of data it is observed that $\sqrt{\overline{u^{{\prime}2}}}/(\sqrt{\overline{u^{{\prime}2}}})_{max}$, (the ratio of RMS velocity fluctuation to maximum RMS velocity fluctuation), is uniquely related with dimensionless distance y/Y', (the ratio of distance normal to splitter plate to the distance where RMS velocity fluctuation is half its maximum value) for all the perforated normal plates. It is interesting to note that for 50% perforation of the normal plate, the RMS pressure fluctuation in the flow field gets reduced to around 60% as compared to that for solid normal plate. Analysis of the results show that the ratio [$C^{\prime}_p$ max/$-C_{pb}(1-{\eta})$], where $C^{\prime}_p$ max is the maximum coefficient of fluctuating pressure, $C_{pb}$ is the coefficient of base pressure and ${\eta}$ is the perforation level (ratio of open to total area), for surface RMS pressure fluctuation levels seems to be constant and has value of about 0.22. Similar analysis show that the ratio $[C^{\prime}_p$ max/$-C_{pb}(1-{\eta})]$ for flow field RMS pressure fluctuation levels seems to be constant and has a value of about 0.32.