• 제목/요약/키워드: 3-D position

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Redistribution of Dopant by Silicidation Treatment in Co/Metal/Si (Co/metal/Si 이중층 구조의 실리사이드화 열처리에 따른 dopant의 재분포)

  • Lee, Jong-Mu;Gwon, Yeong-Jae;Lee, Su-Cheon;Gang, Ho-Gyu;Bae, Dae-Rok;Sin, Gwang-Su;Lee, Do-Hyeong
    • Korean Journal of Materials Research
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    • v.8 no.3
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    • pp.189-194
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    • 1998
  • The redistribution behavior of boron during Co silicidation annealing in the Co/metal/Si system was investigated using SIMS. Ti, Nb and Hf films were used as epitaxy promoting metal layers. After annealing treatment the boron peak height was about 1 order lowered in Co/Ti/Si and Co/Nb/Si systems but the relative peak position from the surface did not change. The distribution of boron was very similar to those of Ti and Nb, because of the strong affinities of boron with them. Also, the position of the main boron peak in the Co/Hf/Si system was almost the same as that of Hf, but the distribution feature of the Co/Hf/Si system somewhat differed from those of Co/Ti/Si and Co/Nb/Si systems. This implies that the affinity between B and Hf is weaker than those of B-Ti and B-Nb. Boron tends to be depleted at the silicidelsi interface while it tends to be piled-up at the Co-metal/Co silicide interface during silicidation annealing.

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Effect of Supplementation with Docosahexaenoic Acid from Gestation to Adulthood on Spatial Learning Performance in Rat (임신기부터 성장기 동안 Docosahexaenoic Acid 보충에 의한 흰쥐의 공간기억력 개선 효과)

  • Lim, Sun-Young
    • Journal of Life Science
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    • v.17 no.10
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    • pp.1400-1405
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    • 2007
  • The effect of supplementation with docosahexaenoic acid into n-3 fatty acid deficient diet on improvement of loaming related brain function was investigated. On the second day after conception, Sprague Dawley strain dams were subjected to a diet containing either n-3 fatty acid deficient (Def) or n-3 fatty acid deficient + docosahexaenoic acid (Def+DHA). After weaning, male pups were fed on the same diet of their respective dams until adulthood. Motor activity and Morris water maze tests were measured at 10 weeks old. In motor activity test, there were no statistically significant differences in moving time and moving distance between the Def and Def+DHA diet groups. The n-3 fatty acid deficient with DHA (Def+DHA) group exhibited a shorter escape latency, swimming time and swimming distance (P<0.05) compared to the n-3 fatty acid deficient group (Def) but there was no difference in resting time and swimming speed between the experimental diet groups. In memory retention trial, the number of crossing of the platform position (region A) was significantly greater than those of other regions for the Def+DHA group. However, the Def group swam randomly without preference for the provisions platform location, indicating poorer memory retention. From those results, supplementation with DHA into the n-3 fatty acid deficient diet improved the spatial loaming ability in rats as assessed by Morris water maze test.

Wall flow characteristics with static mixer position and housing geometry for preventing urea-salt deposition (우레아염 퇴적 방지를 위한 믹서 위치 및 하우징 형상에 따른 벽면 유동특성에 관한 연구)

  • Lee, Banguk;Lee, Jeekeun
    • Journal of Advanced Marine Engineering and Technology
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    • v.37 no.4
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    • pp.368-377
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    • 2013
  • The Urea-SCR system commercialized shows a remarkable performance to reduce NOx emission in heavy duty diesel engines. However, Urea-water solution injected upstream a mixer, which is set up inside a exhaust pipe to promote exhaust gas-atomized droplet mixing, bumps up against the wall of a exhaust pipe as the droplets flow downstream through the exhaust gas. The urea deposited on the wall of the exhaust pipe is changed into the Urea-salt, resulting in the decreased life-time of the SCR catalysts. Therefore, the development of the urea deposition avoidance technologies is being treated as an important issue of the Urea-SCR systems. An experimental study was carried out to investigate the effects of the wall flow characteristics around the mixer-housing assembly with the variation of the mixer housing surrounding and supporting the mixer, which is designed to increase the wall flow and then to reduce droplet deposition. The flow characteristics was investigated by using a hot-wire anemometry for 2-D simplified duct model, and the housing tilt angles and the position of the mixer were changed : angle of $0^{\circ}$, $1^{\circ}$, $2^{\circ}$, $3^{\circ}$, and mixer positions of 0L, 0.5L, 1L. The results showed that the wall flow onto the exhaust pipe was improved with changing the tilt angle of the mixer housing, and the wall flow improved more when the position of the mixer was on 1L.

Finite Element Stress Analysis of Implant Prosthesis of Internal Connection System According to Position and Direction of Load (임플랜트-지대주의 내측연결 시스템에서 하중의 위치 및 경사에 따른 임플랜트 보철의 유한요소 응력분석)

  • Jang, Jong-Seok;Jeong, Yong-Tae;Chung, Chae-Heon
    • Journal of Dental Rehabilitation and Applied Science
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    • v.21 no.1
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    • pp.1-14
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    • 2005
  • The purpose of this study was to assess the loading distributing characteristics of implant prosthesis of internal connection system(ITI system) according to position and direction of load, under vertical and inclined loading using finite element analysis (FEA). The finite element model of a synOcta implant and a solid abutment with $8^{\circ}$ internal conical joint used by the ITI implant was constructed. The gold crown for mandibular first molar was made on solid abutment. Each three-dimensional finite element model was created with the physical properties of the implant and surrounding bone. This study simulated loads of 200N at the central fossa in a vertical direction (loading condition A), 200N at the outside point of the central fossa with resin filling into screw hole in a vertical direction (loading condition B), 200N at the centric cusp in a $15^{\circ}$ inward oblique direction (loading condition C), 200N at the in a $30^{\circ}$ inward oblique direction (loading condition D) or 200N at the centric cusp in a $30^{\circ}$ outward oblique direction (loading condition E) individually. Von Mises stresses were recorded and compared in the supporting bone, fixture, and abutment. The following results have been made based on this study: 1. Stresses were concentrated mainly at the ridge crest around implant under both vertical and oblique loading but stresses in the cancellous bone were low under both vertical and oblique loading. 2. Bending moments resulting from non-axial loading of dental implants caused stress concentrations on cortical bone. The magnitude of the stress was greater with the oblique loading than with the vertical loading. 3. An offset of the vertical occlusal force in the buccolingual direction relative to the implant axis gave rise to increased bending of the implant. So, the relative positions of the resultant line of force from occlusal contact and the center of rotation seems to be more important. 4. In this internal conical joint, vertical and oblique loads were resisted mainly by the implant-abutment joint at the screw level and by the implant collar. Conclusively, It seems to be more important that how long the distance is from center of rotation of the implant itself to the resultant line of force from occlusal contact (leverage). In a morse taper implant, vertical and oblique loads are resisted mainly by the implant-abutment joint at the screw level and by the implant collar. This type of implant-abutment connection can also distribute forces deeper within the implant and shield the retention screw from excessive loading. Lateral forces are transmitted directly to the walls of the implant and the implant abutment mating bevels, providing greater resistance to interface opening.

Diagnosis of Performance Degradation of Direct Methanol Fuel Cell Stack after Long-Term Operation (장기운전에 의한 직접메탄올 연료전지 스택의 성능 열화 분석)

  • Kim, Sang-Kyung;Hyun, Min-Soo;Lee, Byung-Rok;Jung, Doo-Hwan;Peck, Dong-Hyun;Lim, Seong-Yop
    • Korean Chemical Engineering Research
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    • v.49 no.6
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    • pp.775-780
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    • 2011
  • 5-cell DMFC stack was fabricated and operated with the load of 4 A for 4000 hrs. After 4000 hrs operation peak power density of the stack reduced by 27.3%. Two of the five cells did now show performance degradation, the performance of other two was reduced by 40% and the performance of the other decreased by 60%. The amount of performance degradation of each cell by long-term operation did not correlate with the position in the stack. Platinum particle size in the anode catalyst layer of the MEA with the strongest degradation increased and the increase was severer on the position of methanol inlet than on the position of methanol outlet. However, platinum particle size in the cathode catalyst layers did not changed for all the MEA'. Ruthenium crossover from the anode catalyst layer to the cathode catalyst layer through the membrane was observed after 4,000 hrs operation by SEM-EDX and it occurred for all MEA' regardless of the degree of performance degradation. Atomic ratio of ruthenium to platinum in the cathode catalyst layer was the highest in the MEA with the strongest performance degradation.

The Crystal and Molecular Structure of 6-Ethyl-5,6-Dihydrouracil (6-에틸-5,6-디히드로우라실의 결정 및 분자구조)

  • An, Choong Tai
    • Journal of the Korean Chemical Society
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    • v.40 no.3
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    • pp.161-166
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    • 1996
  • 6-ethyl-5,6-dihydrouracil($C_6H_10N_2O_2$) is monoclinic, space group $$P2_{1}c}$$ with a=10.302(2), b=10.419(3), $c=7.095(1)\AA$, $\beta=106.6(0)$, Z=4, $V=729.7(3)\AA$^3$$, $D_c=1.29 g/cm^3,\;{\lambda}(MoK\alpha)=0.71073\AA$, $\mu=0.010cm^{-1}$, F(000)=304, and R=0.054 for 1070 unique observed reflection with F>4.0 $\sigma(F).$ The structure was solved by direct methods and refined by full-matrix least-squares refinement with the fixed C-H bond length at $0.96\AA.$ The hydrouracil molecule makes an envelope conformation with the ethyl substituent oriented to an axial position attainable to a varying degree of steric strain. There are two intermolecular hydrogen-bondings via N-H---O interactions, being nearly parallel to the 100 plane. The shortest distance between molecules is $3.187\AA$ of C(4) and O(8) (-x,-y, 1-z).

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Effects of emotional labor, job stress and burnout on somatization in nurses : In convergence era (융복합 시대의 간호사의 감정노동, 직무스트레스 및 소진이 신체화 증상에 미치는 영향)

  • Oh, Yun Jung;Choi, Young Hee
    • Journal of Digital Convergence
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    • v.13 no.10
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    • pp.415-424
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    • 2015
  • This study was done to identify the influence of emotional labor, job stress and burnout on somatization of nurses live in convergence era. The participants were 387 nurses in D hospital. The average mean score for emotional labor was 3.25, occupational stress was 3.60, burnout was 3.10, and somatization was 2.18. For relations with general characteristics, there was a statistically significant difference in somatization according to age, marital status, educational level, work unit, total clinical career, present department career, position, monthly salary, shift and job satisfaction. Somatization was found to be in a significant positive correlation with emotional labor, occupational stress and burnout. As a result, factor influencing somatization was burnout. This predictor accounted for 29.6% of variance in somatization. The findings of this study showed that burnout was major influencing factor on somatization of nurses. Therefore, it is necessary to develop strategies that can reduce somatization by controlling burnout.

CFD Analysis of EFD-CFD Workshop Case 3 using Commercial and Open Source CFD codes (상용 및 오픈소스 CFD 코드를 이용한 EFD-CFD 워크샵 Case 3 해석)

  • Kim, Jong Rok
    • Journal of the Korean Society for Aeronautical & Space Sciences
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    • v.45 no.3
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    • pp.241-251
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    • 2017
  • Computational fluid dynamics analysis was performed for the case 3 of the EFD-CFD workshop. Solvers were used for three commercial CFD codes(Star-CCM+, Fluent and CFX) and an open source CFD code(SU2). The grid were generated four types depending on the total cells using commercial grid generation code(Pointwise). Mach number of 0.4 and 0.8, 2 degree angle of attack and Mach number of 0.9, 1 degree angle of attack were calculated. Similar pressure coefficient curve and normal force coefficient were showed from the coarse grid to fine grid of four codes. But there is a difference in the drag coefficient. The position of the shock wave was predicted forward as the discretization order increased in calculations using Star-CCM+ and Fluent. The computation time to converge, Fluent, Star-CCM +, CFX are in order, and SU2 takes much time to converge.

3-D vision sensor for arc welding industrial robot system with coordinated motion

  • Shigehiru, Yoshimitsu;Kasagami, Fumio;Ishimatsu, Takakazu
    • 제어로봇시스템학회:학술대회논문집
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    • 1992.10b
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    • pp.382-387
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    • 1992
  • In order to obtain desired arc welding performance, we already developed an arc welding robot system that enabled coordinated motions of dual arm robots. In this system one robot arm holds a welding target as a positioning device, and the other robot moves the welding torch. Concerning to such a dual arm robot system, the positioning accuracy of robots is one important problem, since nowadays conventional industrial robots unfortunately don't have enough absolute accuracy in position. In order to cope with this problem, our robot system employed teaching playback method, where absolute error are compensated by the operator's visual feedback. Due to this system, an ideal arc welding considering the posture of the welding target and the directions of the gravity has become possible. Another problem still remains, while we developed an original teaching method of the dual arm robots with coordinated motions. The problem is that manual teaching tasks are still tedious since they need fine movements with intensive attentions. Therefore, we developed a 3-dimensional vision guided robot control method for our welding robot system with coordinated motions. In this paper we show our 3-dimensional vision sensor to guide our arc welding robot system with coordinated motions. A sensing device is compactly designed and is mounted on the tip of the arc welding robot. The sensor detects the 3-dimensional shape of groove on the target work which needs to be weld. And the welding robot is controlled to trace the grooves with accuracy. The principle of the 3-dimensional measurement is depend on the slit-ray projection method. In order to realize a slit-ray projection method, two laser slit-ray projectors and one CCD TV camera are compactly mounted. Tactful image processing enabled 3-dimensional data processing without suffering from disturbance lights. The 3-dimensional information of the target groove is combined with the rough teaching data they are given by the operator in advance. Therefore, the teaching tasks are simplified

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Photoluminescence Studies of ZnO Nanorods Grown by Vapor Phase Transport (기상이동법으로 성장한 산화아연 나노막대의 포토루미네슨스 분석)

  • Kim, Soaram;Cho, Min Young;Nam, Giwoong;Kim, Min Su;Kim, Do Yeob;Yim, Kwang Gug;Leem, Jae-Young
    • Korean Journal of Metals and Materials
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    • v.49 no.10
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    • pp.818-822
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    • 2011
  • ZnO nanorods were grown on Au-coated Si substrates by vapor phase transport (VPT) at the growth temperature of $600^{\circ}C$ using a mixture of zinc oxide and graphite powders as source material. Au thin films with the thickness of 5 nm were deposited by ion sputtering. Temperature-dependent photoluminescence (PL) was carried out to investigate the optical properties of the ZnO nanorods. Five peaks at 3.363, 3.327, 3.296, 3.228, and 3.143 eV, corresponding to the free exciton (FX), neutral donor bound exciton ($D^{\circ}X$), first order longitudinal optical phonon replica of free exciton (FX-1LO), FX-2LO, and FX-3LO emissions, were obtained at low-temperature (10 K). The intensity of these peaks decreased and their position was red shifted with the increase in the temperature. The FX emission peak energy of the ZnO nanorods exhibited an anomalous behavior (red-blue-red shift) with the increase in temperature. This is also known as an "S-shaped" emission shift. The thermal activation energy for the exciton with increasing temperature in the ZnO nanorods is found to be about 26.6 meV; the values of Varshni's empirical equation fitting parameters are = $5{\times}10^{-4}eV/K$, ${\beta}=350K$, and $E_g(0)=3.364eV$.