• 대한안전경영과학회지
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• 제26권2호
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• pp.87-92
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• 2024

This study aims to compare six observational methods for assessing arm- and hand-intensive tasks, based on literature review. The comparison was conducted in viewpoints of body regions, force/external load, motion repetition, other factors including static posture, coupling, duration/break, pace, temperature, precision task, and final risk or exposure level. The number of risk factors assessed was more, and assessment procedure was more complex than the observational methods for assessing whole-body postural loads such as Ovako Working Posture Analysis System(OWAS), Rapid Upper Limb Assessment(RULA), and Rapid Entire Body Assessment(REBA). Due to these, the intra- and inter-reliabilities were not high. A past study showed that while Hand Arm Risk Assessment Method(HARM) identified the smallest proportion of the work tasks as high risk, Strain Index(SI) and Quick Exposure Check(QEC) hand/wrist were the most rigorous with classifying most work tasks as high risk. This study showed that depending on the observational technique compared, the evaluation factors, risk or exposure level, and evaluation results were different, making it necessary to select a technique appropriate for the characteristics of the work being assessed.

• 한국컴퓨터그래픽스학회논문지
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• 제23권1호
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• pp.9-16
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• 2017

젖은 헤어 또는 동물의 털 시뮬레이션에서 응집력과 강성(stiffness)을 처리하는 것은 어려운 문제이다. 격렬한 움직임을 갖는 헤어나 털이 물에 젖게 되면 끝이 뭉치고 빳빳해지는 현상이 나타나게 되는데, 이는 달리는 동물이나 헤드뱅잉 하는 장면 등에서 쉽게 관찰 할 수 있다. 기존의 방법들은 정해진 시뮬레이션 시나리오에서 이 문제를 해결하려고 했지만 여전히 젖은 헤어의 특징을 묘사하기 위한 일반적인 방법이 존재하지 않는다. 이 문제를 해결하기 위해 우리는 응집력과 강성에 대한 새로운 모델링 방법을 제안한다. 기존 연구들은 물이 모발에 흡수되는 현상을 모델링 하는데 초점을 맞춘 반면, 우리는 젖은 모발의 움직임을 사실적으로 표현하는데 집중한다. 젖은 헤어는 마른 헤어와는 다르게 인접한 모발들끼리 응집력이 작용하여 서로 뭉치는 형태를 띄며, 물의 포화도가 높아질수록 빳빳해지는 독특한 물리적 특성이 나타난다. 제안된 기법의 핵심은 SPH (smoothed particle hydrodynamics) 기반의 표면 장력 모델을 확장하여 응집력을 표현하고, 강성 제약을 두어 모발의 탄성력을 조절하는 것이다. 우리 기법은 젖은 모발이 격렬한 움직임에서도 응집력을 잘 유지할 수 있도록 도와주며, 물의 포화도에 따른 모발의 빳빳함을 표현하여 사실적인 젖은 헤어 시뮬레이션 결과를 보여준다.

• Ocean and Polar Research
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• 제30권3호
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• pp.303-312
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• 2008

Despite the impacts of the climate changes on the pelagic ecosystem, few studies have examined the pelagic-benthic coupling in the adjacent East China Sea and Korea Strait. Therefore, the species composition and abundance of the macrobenthic community, as well as the potential food sources of benthic fauna were investigated in the present study using stable isotope analysis (${\delta}^{13}C\;and\;{\delta}^{15}N$) for suspended particulate organic matter (SPOM), sedimentary organic matter (SOM), phytoplankton, and zooplankton. A total of 157 macrobenthic fauna were collected, and the density of the macrobenthic fauna ranged from 4 to 434 ind./0.25 $m^2$, with an average density of 149 ind./0.25 $m^2$. The density of the benthic fauna increased moving from offshore shelf sites to coastal sites adjacent to the Korea Strait. Cluster analysis showed that the macrobenthic communities consisted of three distinct groups: group A in the Korea Strait, group B in the East China Sea, and group C near Ieodo. The dominant species in group A were the amphipods Photis japonica and Ampelisca miharaensis, followed by the polychaete Scolotoma longifolia. Environmental variables, such as the temperature of the seawater and sediment, and oxygen, and chlorophyll a levels, appeared to affect the structure of the community, suggesting the importance of coupling with the pelagic system. The ${\delta}^{13}C$ values of SPOM and zooplankton ranged from -22.97 to -23.5% and -19.92 to -21.86%, respectively, showing a relatively narrow range(<1%) between the two components. The difference between the ${\delta}^{13}C$ values of SOM and pelagic organic matter was also within 1%, suggesting that the SOM originated from the pelagic system, which is an important factor controlling the macrobenthic community.

• 한국자기학회지
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• 제7권3호
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• pp.152-158
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• 1997

Ni$_{66}$Fe$_{16}$ $Co_{18}$ /Cu/Co 삼층막을 4 .deg. tilt-cut Si(111) 기판과 Cu(50 .angs. ) 바닥층 위에 형성하고, 사진식각 및 에칭 작업을 통해 자기저항 메모리 소자를 제작하여 자기저항 메모리 특성을 연구하였다. 외부 자장의 인가 없이 증착한 NiFeCo/Cu/Co 삼층막은 4 .deg. tilt-cut Si(111) 기판과 Cu(50 .angs. ) 바닥층의 영향으로 면내 일축자기이방성을 형성하였으며, 낮은 자장 내에서 높은 자기저항비와 자기저항민감도 등 자기저항 메모리 소자에 응용이 가능한 우수한 자기저항 특성을 나타내었다. NiFeCo/Cu/Co 삼층막의 Cu 사잇층 두께 변화에 따라 삼층막을 이루는 두 자성층 간에 강자성 및 반강자성 결합력이 관찰되었으며, 결합력은 사잇층 두께에 민감하게 변화하여 NiFeCo/Cu/Co 삼층막의 메모리 특성에 영향을 끼쳤다. 사잇층 두께의 변화에 대해 최적화된 [NiFeCo(60 .angs. )/Cu(25 .angs. )/Co(30 .angs. )]/Cu(50 .angs. )/Si(111, 4 .deg. tilt-cut) 스핀밸브 삼층막을 이용하여 거시적 자기저항 메모리 소자를 제작하고, 시험 소자의 메모리 동작에 대해 관찰하였다. Sense 전류는 10 mA로 고정하고, 약 5 * $10^{5}$ A/$cm^{2}$의 word 전류를 가해 약 10 mV의 출력 전압을 시험 소자에서 얻었으며, NiFeCo/Cu/Co 스핀밸브 삼층막의 자기저항 메모리 소자에의 응용 가능성을 확인할 수 있었다.다.

• 한국자기학회지
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• 제11권5호
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• pp.184-188
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• 2001

DC-스퍼터를 이용하여 기판온도를 실온과 20$0^{\circ}C$로 변화시켜 , 균일한 내부구조를 갖는 구조와 결정립내부에 미세한 자가정렬나노구조(SONS)를 갖는 Co-22%Cr 합금 박막을 각각 제조하고 이들의 미세구조와 도메인구조를 투과전자현미경(TEM)과 자기력현미경(MFM)을 이용하여 확인하였다. Co가 먼저 부식되도록 조치하고 관찰한 투과전자현미경 결과, 실온에서 제작된 박막의 경우에는 결정립 내부가 균일한 조성을 보인 반면, 기판온도가 20$0^{\circ}C$인 Co-22%Cr합금 박막은 결정립 내부에 SONS를 형성하여 판상의 미세 Co-과잉상을 가지는 특이한 미세구조를 가지는 것을 확인하였다. 자기력현미경에 의해 확인된 결과, SONS가 없는 시편(기판온도를 실온으로 유지한 경우)은 주기 5000 정도의 미로형 도메인(domains)이 생겼다. 미로형 도메인은 결정간의 교환에너지가 큰 경우 발생하는 구조로서 고밀도 자기기록이 불리할 것이 예상되었다. 이와 비교해서 SONS가 생성된 (기판온도를 20$0^{\circ}C$로 유지한 경우)시편은 주기 500 정도의 매우 미세한 구형 도메인을 보였다. 미세구형 도메인은 각 도메인간의 교환에너지가 작아 열적 변화에도 데이터가 안정하므로 고밀도 기록에 유리하다고 예상되었다.

• Steel and Composite Structures
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• 제47권1호
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• pp.91-102
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• 2023

To study the evaluation standard and control limit of mortar filling layer void length, in this paper, the train sub-model was developed by MATLAB and the track-bridge sub-model considering the mortar filling layer void was established by ANSYS. The two sub-models were assembled into a train-track-bridge coupling dynamic model through the wheel-rail contact relationship, and the validity was corroborated by the coupling dynamic model with the literature model. Considering the randomness of fastening stiffness, mortar elastic modulus, length of mortar filling layer void, and pier settlement, the test points were designed by the Box-Behnken method based on Design-Expert software. The coupled dynamic model was calculated, and the support vector regression (SVR) nonlinear mapping model of the wheel-rail system was established. The learning, prediction, and verification were carried out. Finally, the reliable probability of the amplification coefficient distribution of the response index of the train and structure in different ranges was obtained based on the SVR nonlinear mapping model and Latin hypercube sampling method. The limit of the length of the mortar filling layer void was, thus, obtained. The results show that the SVR nonlinear mapping model developed in this paper has a high fitting accuracy of 0.993, and the computational efficiency is significantly improved by 99.86%. It can be used to calculate the dynamic response of the wheel-rail system. The length of the mortar filling layer void significantly affects the wheel-rail vertical force, wheel weight load reduction ratio, rail vertical displacement, and track plate vertical displacement. The dynamic response of the track structure has a more significant effect on the limit value of the length of the mortar filling layer void than the dynamic response of the vehicle, and the rail vertical displacement is the most obvious. At 250 km/h - 350 km/h train running speed, the limit values of grade I, II, and III of the lengths of the mortar filling layer void are 3.932 m, 4.337 m, and 4.766 m, respectively. The results can provide some reference for the long-term service performance reliability of the ballastless track-bridge system of HRS.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2013년도 제44회 동계 정기학술대회 초록집
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• pp.334-334
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• 2013

In the past decade, the infrared detectors based on intersubband transition in quantum dots (QDs) have attracted much attention due to lower dark currents and increased lifetimes, which are in turn due a three-dimensional confinement and a reduction of scattering, respectively. In parallel, focal plane array development for infrared imaging has proceeded from the first to third generations (linear arrays, 2D arrays for staring systems, and large format with enhanced capabilities, respectively). For a step further towards the next generation of FPAs, it is envisioned that a two-dimensional metal hole array (2D-MHA) structures will improve the FPA structure by enhancing the coupling to photodetectors via local field engineering, and will enable wavelength filtering. In regard to the improved performance at certain wavelengths, it is worth pointing out the structural difference between previous 2D-MHA integrated front-illuminated single pixel devices and back-illuminated devices. Apart from the pixel linear dimension, it is a distinct difference that there is a metal cladding (composed of a number of metals for ohmic contact and the read-out integrated circuit hybridization) in the FPA between the heavily doped gallium arsenide used as the contact layer and the ROIC; on the contrary, the front-illuminated single pixel device consists of two heavily doped contact layers separated by the QD-absorber on a semi-infinite GaAs substrate. This paper is focused on analyzing the impact of a two dimensional metal hole array structure integrated to the back-illuminated quantum dots-in-a-well (DWELL) infrared photodetectors. The metal hole array consisting of subwavelength-circular holes penetrating gold layer (2DAu-CHA) provides the enhanced responsivity of DWELL infrared photodetector at certain wavelengths. The performance of 2D-Au-CHA is investigated by calculating the absorption of active layer in the DWELL structure using a finite integration technique. Simulation results show the enhanced electric fields (thereby increasing the absorption in the active layer) resulting from a surface plasmon, a guided mode, and Fabry-Perot resonances. Simulation method accomplished in this paper provides a generalized approach to optimize the design of any type of couplers integrated to infrared photodetectors.

• 한국환경과학회지
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• 제26권2호
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• pp.231-238
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• 2017

Rapid industrial development has led to a serious problem of pollution in the industrial sector. With the increasing social need for environmental protection, research on air pollution prevention equipment for reducing pollutants in industrial processes is actively being undertaken. The deterioration of existent, installed facilities, their increased emission rates, and the strengthening of the effluent quality standards make complying with permissible emission standards difficult. In fact, installing new electric precipitators or complementing existent facilities is inevitable. The expansion and complementation of the installed electrical precipitators have led to improvements in dust collection efficiency, shorter working times, and lower costs. Because of its easy installation and simple manufacturing process, the production method with the discharge electrode of an electric precipitator is widely used. The following conclusions were reached by classifying discharge electrodes into four types based on the production method and mutually comparing them by their dust collection efficiency. None of the four types used in this study were damaged by impact. However, we were able to confirm some strain from the compression sites of both type A and type B. Both type B and type C are expected to have greater dust collection efficiencies than the other models due to their large vibration transmissibility. Moreover, the high vibrational energy is expected to cause rapping damage during its operation. Particularly, in the case of type B, some of the strain was found at the end of the compression site. The coupling schemes of both type C and type D are out of vibration transmissibility. On the other hand, the ability to maintain straightness and solidity of the side is regarded as outstanding and stable. Type D has outstanding on-site workability, considering the presence of locking, structural stability, and work conditions. From these experiments, we determined that type C is the most ideal connection method of discharge electrode, considering its construction period of renovation. Type C is inferior to type D with regard to on-site workability. However, type C has outstanding dedusting transmission with regard to the straightness, solidity maintenance, and vibration of shearing stress.

• Wind and Structures
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• 제28권2호
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• pp.71-87
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• 2019

The yaw and interference effects of blades affect aerodynamic performance of large wind turbine system significantly, thus influencing wind-induced response and stability performance of the tower-blade system. In this study, the 5MW wind turbine which was developed by Nanjing University of Aeronautics and Astronautics (NUAA) was chosen as the research object. Large eddy simulation on flow field and aerodynamics of its wind turbine system with different yaw angles($0^{\circ}$, $5^{\circ}$, $10^{\circ}$, $20^{\circ}$, $30^{\circ}$ and $45^{\circ}$) under the most unfavorable blade position was carried out. Results were compared with codes and measurement results at home and abroad, which verified validity of large eddy simulation. On this basis, effects of yaw angle on average wind pressure, fluctuating wind pressure, lift coefficient, resistance coefficient,streaming and wake characteristics on different interference zone of tower of wind turbine were analyzed. Next, the blade-cabin-tower-foundation integrated coupling model of the large wind turbine was constructed based on finite element method. Dynamic characteristics, wind-induced response and stability performance of the wind turbine structural system under different yaw angle were analyzed systematically. Research results demonstrate that with the increase of yaw angle, the maximum negative pressure and extreme negative pressure of the significant interference zone of the tower present a V-shaped variation trend, whereas the layer resistance coefficient increases gradually. By contrast, the maximum negative pressure, extreme negative pressure and layer resistance coefficient of the non-interference zone remain basically same. Effects of streaming and wake weaken gradually. When the yaw angle increases to $45^{\circ}$, aerodynamic force of the tower is close with that when there's no blade yaw and interference. As the height of significant interference zone increases, layer resistance coefficient decreases firstly and then increases under different yaw angles. Maximum means and mean square error (MSE) of radial displacement under different yaw angles all occur at circumferential $0^{\circ}$ and $180^{\circ}$ of the tower. The maximum bending moment at tower bottom is at circumferential $20^{\circ}$. When the yaw angle is $0^{\circ}$, the maximum downwind displacement responses of different blades are higher than 2.7 m. With the increase of yaw angle, MSEs of radial displacement at tower top, downwind displacement of blades, internal force at blade roots all decrease gradually, while the critical wind speed decreases firstly and then increases and finally decreases. The comprehensive analysis shows that the worst aerodynamic performance and wind-induced response of the wind turbine system are achieved when the yaw angle is $0^{\circ}$, whereas the worst stability performance and ultimate bearing capacity are achieved when the yaw angle is $45^{\circ}$.

• Journal of Magnetics
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• 제7권3호
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• pp.72-79
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• 2002

Local M-H loops have been measured on the free layer of a tunneling magnetoresistance (TMR) junction using the magneto-optical Kerr effect (MOKE) system, with an optical beam size of about 2 $\mu$m diameter. Tunnel junctions were deposited using the DC magnetron sputtering method in a chamber with a base pressure of 3$\times$10$^{-9}$ Torr. The relatively irregular variations of coercive force H$_c$(∼17.5 Oe) and unidirectional anisotropy field H$_{ua}$(∼7.5 Oe) in the as-deposited sample are revealed. After $200{^{\circ}C}$ annealing, He decreases to 15 Oe but H$_{ua}$ increases to 20 Oe with smooth local variations. Two-dimensional plots of H$_c$ and H$_{ua}$ show the symmetric saddle shapes with their axes aligned with the pinned layer, irrespective of the annealing field angle. This is thought to be caused by geometric effects during deposition, together with a minor annealing effect. In addition, the variation of root mean square (RMS) surface roughness reveals it to be symmetric with respect to the center of the pinned-layer axis, with the roughness of 2.5 $\AA$ near the edge and 5.8 $\AA$ at the junction center. Comparison of surface roughness with the variation of H$_{ua}$ suggests that the H$_{ua}$ variation of the free layer is well described by dipole interactions related to surface roughness. As a whole, the reversal magnetization is not uniform over the entire junction area and the macroscopic properties are governed by the average sum of local distributions.