• 제목/요약/키워드: average film thickness

검색결과 187건 처리시간 0.031초

X-Ray Reflectivity Analysis Incorporated with Genetic Algorithm to Analyze the Y- to X Type Transition in CdA LB Film

  • 최정우;조경상;이희우;이원홍;이한섭
    • Bulletin of the Korean Chemical Society
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    • 제19권5호
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    • pp.549-553
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    • 1998
  • The structure and layer distribution of cadmium arachidate Langmuir-Blodgett film were analyzed by the small angle X-ray reflectivity measurements using synchrotron radiation. Y-to X type transition was ocurred during the 39th passage of deposition of cadmium arachidate. Based on the measurement of the consumed area of the monolayer, it was determined that about 27.5 layer was deposited. Using the synchrotron X-ray, the reflectivity profile of cadmium arachidate LB film over the wide range of grazing angle was obtained. The X-ray reflectivity profile was analyzed using the recursion formula. By fitting the location and dispersion of the subsidiary maxima between the Bragg peaks of the measured reflectivity profile with that of the calculated reflectivity profile, the average thickness and the distribution of layer thickness were evaluated. The genetic algorithm was adopted to the fitting of reflectivity profile to evaluate the optimum value of the number distribution of layer. Based on the morphology measurement with an atomic force microscopy (AFM), the domain structure and mean roughness of LB films were obtained. The mean roughness value calculated based on the number of layer distribution obtained from the measurement by AFM is consistent with that obtained from X-ray reflectivity analysis.

파이어링 상태의 일정 축 각속도에서 엔진베어링의 마모 해석 - Part II: 저어널베어링 마모 계산 (Wear Analysis of Engine Bearings at Constant Shaft Angular Speed during Firing State - Part II: Calculation of the Wear on Journal Bearings)

  • 전상명
    • Tribology and Lubricants
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    • 제34권4호
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    • pp.146-159
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    • 2018
  • This paper presents a wear analysis procedure for calculating the wear of journal bearings of a four-strokes and four-cylinder engine operating at a constant angular crank shaft speed during firing conditions. To decide whether the lubrication state of a journal bearing is in the possible region of wear scar, we utilize the concept of the centerline average surface roughness to define the most oil film thickness scarring wear (MOFTSW) on two rough surfaces. The wear volume is calculated from the wear depth and wear angle, determined by the magnitude of each film thickness on a set of oil films with thicknesses lower than the MOFTSW at every crank angle. To calculate the wear volume at one contact, the wear range ratio during one cycle is used. The total wear volume is then determined by accumulating the wear volume at every contact. The fractional film defect coefficient, asperity load sharing factor, and modified specific wear rate for the application of the mixed-elasto-hydrodynamic lubrication regime are used. The results of this study show that wear occurs only at the connecting-rod big-end bearing. Thus, simulation results of only the big-end bearing are illustrated and analyzed. It is shown that the wear volume of each wear scar group occurs consecutively as the crank angle changes, resulting in the total accumulated wear volume.

유방조직등가 팬텀을 이용한 Screen-Film과 Digital Mammography에서의 평균 유선선량 (Comparison of Average Glandular Dose in Screen-Film and Digital Mammography Using Breast Tissue-Equivalent Phantom)

  • 신귀순;김정민;김유현;최종학;김창균
    • 대한방사선기술학회지:방사선기술과학
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    • 제30권1호
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    • pp.13-23
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    • 2007
  • 유방촬영장치가 screen-film system에서 최근에는 빠른 속도로 digital system으로 교체되고 있는 추세이다. Digital system이 screen-film system에 비해 여러 가지 장점을 가지고 있다. 그 중의 하나가 digital detector가 screen-film보다 X선 흡수효율이 더 높으며, digital system 중에서도 direct digital detector가 indirect digital detector보다 흡수효율이 높다. 이에 입각하면 촬영 시 적은 선량을 주어도 되기 때문에 환자피폭선량이 감소한다. 그러나 임상 방사선사들이 느끼는 바는 달랐다. 따라서 이번 연구에서는 screen-film mammography system, computed mammography system, indirect digital mammography system, direct digital mammography system에서 glandularity가 30%, 50% 및 70%인 세 종류의 유방조직 등가팬텀을 이용하여 평균유선선량(AGD)을 측정하여 다음과 같은 결론을 얻었다. Screen-film보다 digital detector가 X선 흡수효율이 높지만, glandularity가 30%인 경우의 AGD는 오히려 SFM에서 가장 낮았고, 그다음 CM, IDM, DDM 순으로 증가되었다. 자동노출장치로 설정하였지만 두께나 glandularity에 따라 target/filter의 조합이 바뀌지 않고 Mo/Mo으로 계속 사용된 SFM에서는 AGD가 급격히 증가되었다. 따라서 높은 glandularity를 가진 두꺼운 팬텀을 위한 고에너지 촬영에서는 SFM에서 AGD값이 가장 높았고, 저에너지 촬영에서는 DDM에서 AGD값이 가장 높았다. 그러나 target/filter의 조합이 다양하게 바뀐 CM에서는 두께나 glandularity에 따른 AGD의 곡선이 가장 완만하게 증가하였으며, AGD값이 가장 낮았다. 이와 같이 두께와 glandularity가 증가함에 따라 target/filter의 조합이 Mo/Mo에서 Mo/Rh으로 더 증가하면 Rh/Rh으로 바뀌는 것이 AGD의 증가량이 적어 환자의 피폭선량 측면에서 바람직하다. 따라서 유방촬영에서 환자의 피폭선량을 평가하기 위해서는 검출효율 외에도 여러 가지 촬영 변수가 중요한 역할을 한다.

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'부유' 단감 MAP 저장에서 과실 크기에 따른 PE 필름 봉지의 적정 규격 (Optimal Dimension of PE Film Bag According to Fruit Size in MAP Storage of 'Fuyu' Persimmon Fruit)

  • 이용재
    • 한국식품과학회지
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    • 제36권5호
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    • pp.733-739
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    • 2004
  • 과실의 연화 및 변색이 가장 적게 발생되는 과실 크기별 봉지 규격을 구명하고 이와 더불어 연화 및 변색과 상관관계를 가지는 봉지 내 산소와 이산화탄소 농도와의 관계를 이용하여, 최적 기체 농도가 이루어지도록 PE 필름 봉지의 적정 규격을 모델링하고자 하였다. 다섯 등급으로 선과된 과실(LL:261g, L:217g, M:188g, S:168g, SS:154g)을 작업성과 미관을 고려하여 과실과 봉지 사이의 간격을 1-1.5cm 되게 PE 필름 봉지를 적용시켰을 때, LL은 150mm, L은 140mm, M과 S는 130mm, SS는 120mm의 봉지 폭에 각각 376mm, 357mm, 344mm, 333mm, 318mm의 봉지 길이가 적절하였다. 연화 및 흑변과 갈변 발생을 최소화하는 봉지 내 산소와 이산화탄소 농도는 각각 0.5-1.0%와 6.0-8.0%였으며, 이를 유지할 수 있는 과실 크기별 PE 필름 봉지의 최적두께는 LL은 $45{\mu}m$, L은 $50{\mu}m$, M은 $55{\mu}m$, S는 $60{\mu}m$, SS는 $65{\mu}m$로 조사되었다. 주어진 과실 크기에 맞는 봉지의 면적$(mm^2)$은 과실의 중량(g)에 대한 2차 단순회귀$(Y=-4055.707+627.993X_1-0.701{X_1}^2)$가 매우 적합하였고, 이 때 PE 필름 봉지 내에 원하는 수준의 산소나 이산화탄소 농도(Y, %)를 유지할 수 있는 PE 필름의 두께를 구하는 회귀식은 과실 중량$(X_1,\;g)$과 봉지 두께$(X_2,\; {\mu}m)$의 선형 중회귀$(O_2:Y=5.798-0.0109X_1-0.0491X_2,\;CO_2:Y=-2.427+0.01927X_l+0.09646X_2)$가 가장 적합하였다.

유기 반도체 CuPccp LB초박막의 제작 및 특성 (Fabrication and Properties of Organic Semiconductor CuPccp LB Thin Film)

  • 조민재;쑤양싸이양;이진수;안다현;정치섭
    • 센서학회지
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    • 제28권1호
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    • pp.23-29
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    • 2019
  • A copper tetracumylphenoxy phthalocyanine (CuPccp) thin film was formed on an organic insulator film by Langmuir-Blodgett (LB) deposition for gas sensor fabrication. To increase the reproducibility of film transfer, stearyl alcohol was used as a transfer promoter. The structural properties of the CuPccp layers were optically monitored through attenuated total reflection and polarization-modulated ellipsometry techniques. The average thickness of a single layer of the CuPccp LB film was measured to be 2.5 nm. Despite the role of the transfer promoter, the stability of the layer transfer was not sufficient to ensure homogeneity of the LB film. This was probably due to the presence of aggregates in the molecular structure of the CuPccp LB film. Nevertheless, copper phthalocyanine polymorphism can be greatly suppressed by the LB arrangement, which appears to contribute to the improvement of electrical conductivity. The p-type semiconductor characteristics were confirmed by Hall measurements from the CuPccp LB films.

Evaluation of Tear Film Lipid Layer Thickness Measurements Obtained Using an Ocular Surface Interferometer in Nasolacrimal Duct Obstruction Patients

  • Lee, Sang Min;Chung, Sok Joong;Lew, Helen
    • Korean Journal of Ophthalmology
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    • 제32권6호
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    • pp.445-450
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    • 2018
  • Purpose: To compare the tear film lipid layer thickness (LLT) between patients with incomplete nasolacrimal duct obstruction (NLDO) and normal controls and to analyze the changes in tear film LLT and blinking pattern after silicone tube intubation in NLDO patients. Methods: We reviewed the medical records of 68 eyes in 52 incomplete NLDO patients who underwent silicone tube intubation from January 2017 to July 2017. The LLT, blinking pattern, and Meibomian gland image were measured with the LipiView II ocular surface interferometer. The Meibomian gland drop-out ratio was measured using the polygon selection tool in the Image J program. Tear meniscus height, which is the other lacrimal indicator, was assessed with spectral-domain optical coherence tomography. Results: Tear meniscus height was significantly decreased after silicone tube intubation (p < 0.01). Preoperative minimum, maximum, and average LLT values were $62.4{\pm}24.0$, $86.7{\pm}17.9$, and $71.7{\pm}23.3nm$, respectively. Significant changes in the minimum, maximum, and average LLT ($74.8{\pm}23.6$, $98.8{\pm}11.0$, and $91.6{\pm}16.1nm$, respectively) were observed after silicone tube intubation (p < 0.001, p = 0.001, and p < 0.001). The partial blinking/total blinking ratio in 20 seconds and the Meibomian gland drop-out ratio showed no significant change after silicone tube intubation. Conclusions: Overall, the LLT was increased after silicone tube intubation. Silicone tube intubation may be helpful in maintaining LLT with a normalized of amount of tears.

수소화된 비정질 실리콘 박막을 이용한 웨이퍼 패시베이션 특성 연구 (A study on wafer surface passivation properties using hydrogenated amorphous silicon thin film)

  • 이승직;김기형;오동해;안황기
    • 한국신재생에너지학회:학술대회논문집
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    • 한국신재생에너지학회 2010년도 추계학술대회 초록집
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    • pp.46.1-46.1
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    • 2010
  • Surface passivation of crystalline silicon(c-Si) surface with a-Si:H thin films has been investigated by using quasi-steady-state photo conductance(QSSPC) measurements. Analyzing the influence of a-Si:H film thickness, process gas ratio, deposition temperature and post annealing temperature on the passivation properties of c-Si, we optimized the passivation conditions at the substrate temperature of $200-250^{\circ}C$. Best surface passivation has been obtained by post-deposition annealing of a-Si:H film layer. Post annealing around the deposition temperature was sufficient to improve the surface passivation for silicon substrates. We obtained effective carrier lifetimes above 5.5 ms on average.

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틸팅패드 스러스트베어링의 모멘트평형에 대한 고찰 (On Moment Balance of Tilting-Pad Thrust Bearings)

  • 김호종;최성필;하현천
    • 한국윤활학회:학술대회논문집
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    • 한국윤활학회 2003년도 학술대회지
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    • pp.261-266
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    • 2003
  • The present paper theoretically investigates characteristics of moment balance of a tilting-pad thrust bearing. Pressure of lubricant film of the bearing was computed using tile finite element method, and average film temperature was estimated from the heat balance over a pad. From the investigation, it has been found that different two sets of tilt angles satisfy moment equilibrium of the pad about tile pivot for a given pivot location. The tilt angles converged depend upon initial tilt angles assumed. Quite different bearing performance, including load capacity, film thickness, and temperature, is shown to be obtained based on choice of the initial tilt angles.

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Double Textured AZO Film and Glass Substrate by Wet Etching Method for Solar Cell Application

  • 정원석;남상훈;부진효
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2012년도 제42회 동계 정기 학술대회 초록집
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    • pp.594-594
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    • 2012
  • Al doped ZnO (AZO) thin films were deposited on textured glass substrate by magnetron sputtering method. Also, AZO films on textured glass were etched by hydrochloric acid (HCl). Average thickness of etched AZO films are 90 nm. We observed morphology of AZO film by AFM with various etchant concentration and etching time. Etched AZO films have low resistivity and high haze. The surface RMS roughness of AZO film was increased from 53.8 nm to 84.5 nm. The haze ratio was also enhanced in above 700 nm of wavelength due to light trapping effect was increased by rough AZO surface. The etched AZO films on textured glass are applicable to fabricate solar cell.

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틸팅패드 스러스트베어링의 모멘트평형에 대한 고찰 (On Moment Balance of Tilting-Pad Thrust Bearings)

  • 김호종;최성필;하현천
    • Tribology and Lubricants
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    • 제20권3호
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    • pp.152-156
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    • 2004
  • The present paper theoretically investigates characteristics of moment balance of a tilting-pad thrust bearing. Pressure of lubricant film of the bearing was computed using the finite element method, and average film temperature was estimated from the heat balance over a pad. From the investigation, it has been found that different two sets of tilt angles satisfy moment equilibrium of the pad about the pivot for a given pivot location. The tilt angles converged depend upon initial tilt angles assumed. Quite different bearing performance, including load capacity, film thickness, and temperature, is shown to be obtained based on choice of the initial tilt angles.