• 제목/요약/키워드: 3D surface profile

검색결과 183건 처리시간 0.028초

거푸집 종류에 따른 콘크리트 표면 특성 (Surface Characteristics of Concrete According to Types of Formworks)

  • 박세언;최정일;이봉기;이방연
    • 한국건설순환자원학회논문집
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    • 제9권4호
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    • pp.499-505
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    • 2021
  • 이 연구의 목적은 거푸집 종류별로 콘크리트 표면의 물리/화학적 특성을 실험적으로 조사하는 것이다. 이를 위하여 건설공사에 일반적으로 사용되는 합판 거푸집과 코팅된 합판 거푸집을 준비하였고, 추가로 콘크리트 표면 열화나 거친 표면을 모사하기 위해 사포를 부착한 합판 거푸집을 준비하였다. 콘크리트는 일반 콘크리트를 사용하였다. 콘크리트 표면 특성은 육안관찰, 주사전자현미경 관찰, 성분 이미지 맵핑, 화학성분 분석, 2차원과 3차원 표면 형상 분석, 그리고 제타 전위 측정을 통해 조사하였다. 실험결과 코팅된 거푸집과 접한 콘크리트 표면이 가장 매끄럽고, 사포를 부착한 거푸집과 접한 콘크리트 표면이 가장 거친 것으로 나타났다. 이외에도 거푸집 종류별로 표면 특성에 뚜렷한 차이가 나타났다. 다만 표면 거칠기가 화학 성분이나 제타 전위에 비하여 차이가 크게 나타났다.

다공성 매질이 존재하는 용광로 내부 이상유체 경계면의 특성 (CHARACTERISTICS OF INTERFACE BETWEEN TWO-PHASE FLUIDS FLOW IN A FURNACE WITH POROUS MEDIUM)

  • 박경민;이동조;이정호;윤현식
    • 한국전산유체공학회지
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    • 제21권1호
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    • pp.110-116
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    • 2016
  • The present study numerically investigated the deformation of the interface of two-phase fluids flow in a blast furnace. To simulate three-dimensional(3D) incompressible viscous two-phase flow in the furnace filled with the air and molten iron, the volume of fluid(VOF) method based on the finite volume method has been utilized. In addition, the porous medium with the porosity has been considered as the bed of the particles such as cokes and char etc. For the comparison, the single phase flow and the two-phase flow without the porosity have been simulated. The two-phase flow without porosity condition revealed the smooth parabolic profile of the free surface near the outlet. However, the free surface under the porosity condition formed the viscous finger when the free surface was close to the outlet. This viscous finger accelerated the velocity of the free surface falling and the outflow velocity of the fluids near the outlet.

레이저묘화 기술을 이용한 3차원 미세구조물 제조 (Fabrication of three dimensional microstructures using laser direct writing technique)

  • 정성호;한성일
    • 한국정밀공학회:학술대회논문집
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    • 한국정밀공학회 2003년도 춘계학술대회 논문집
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    • pp.670-673
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    • 2003
  • Fabrication of three dimensional microstructures by laser-assisted chemical vapor deposition of material is investigated. To fabricate microstructures, a thin layer of deposit in desired patterns is first written using laser direct writing technique and on top of this layer a second layer is deposited to provide the third dimension normal to the surface. By depositing many layers. a three dimensional microstructure is fabricated. Optimum deposition conditions for direct writing of initial and subsequent layers with good surface quality and profile uniformity are determined. Using an arson ion laser and ethylene as the light source and reaction gas, respectively, fabrication of three-dimensional carbon microstructures is demonstrated.

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로봇 롤러 헤밍의 유한요소해석 (Finite Element Analysis of the Robot Roller Hemming)

  • 주석재;강민준
    • 대한기계학회:학술대회논문집
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    • 대한기계학회 2008년도 추계학술대회A
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    • pp.475-480
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    • 2008
  • Hemming, especially curl hemming, is required along the wheel housing for safety. Robot roller hemming is suitable for it. In this paper, both the flat hemming and the curl hemming along either the straight profile or the curved profile are analyzed using finite element program MSC.Marc to verify the hemming test results. Both the inner panel and the outer panel are modeled using 3-D solid elements and the roler is modeled using rigid surface. In the curl hemming, there is a case that the curl is not formed if the pre-hemming force is not sufficient. It agrees with the test results.

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EPMA를 이용한 침탄강의 정확하고 신뢰성 있는 탄소농도 측정을 위한 분석조건 최적화 (Optimization of Analytical Condition for Reliable and Accurate Measurement of Carbon Concentration in Carburized Steel by EPMA)

  • 권기훈;박현준;최병호;이영국;문경일
    • 한국재료학회지
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    • 제33권3호
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    • pp.106-114
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    • 2023
  • The carbon concentration in the carburized steels was measured by electron probe microanalysis (EPMA) for a range of soluted carbon content in austenite from 0.1 to 1.2 wt%. This study demonstrates the problems in carbon quantitative analysis using the existing calibration curve derived from pure iron (0.008 wt%C) and graphite (99.98 wt%C) as standard specimens. In order to derive an improved calibration curve, carbon homogenization treatment was performed to produce a uniform Kα intensity in selected standard samples (AISI 8620, AISI 4140, AISI 1065, AISI 52100 steel). The trend of detection intensity was identified according to the analysis condition, such as accelerating voltage (10, 15, 30 keV), and beam current (20, 50 nA). The appropriate analysis conditions (15 keV, 20 nA) were derived. When the carbon concentration depth profile of the carburized specimen was measured for a short carburizing time using the improved calibration curve, it proved to be a more reliable and accurate analysis method compared to the conventional analysis method.

탄소입자 치료 시 열가소성 고정기구의 공기층에 따른 선량 변화 평가 (Evaluation of Dose Variation according to Air Gap in Thermoplastic Immobilization Device in Carbon Ion)

  • 나예진;장지원;장세욱;박효국;이상규
    • 대한방사선치료학회지
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    • 제35권
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    • pp.33-39
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    • 2023
  • 목 적: 환자 체표면과 고정기구 사이에 발생하는 공기층 두께에 따른 선량 변화를 치료 계획을 통해 알아보고자 한다. 대상 및 방법: 팬텀과 열가소성 고정기구 사이에 5 mm 두께의 Bolus를 0, 1, 2, 3장을 놓아 공기층의 두께를 조절하였고 고정기구를 씌워 총 4가지 조건으로 전산화 모의단층촬영을 시행하였다. 430 cGy (Relative Biological Effectiveness,RBE)씩 6번이 조사 되도록 계획하였으며, 임상표적체적의 95% 부피에 전달된 선량이 2580 cGy (RBE)가 되도록 치료 계획을 수립하였다. 임상표적체적의 선량은 Lateral dose profile의 반치폭값으로 평가하였고 피부 선량은 선량 체적 곡선으로 평가하였다. 결 과: 임상표적체적에서 Lateral dose profile 반치폭 값은 4.89, 4.86, 5.10, 5.10 cm로 나타났다. 피부에서 4가지 조건의 선량의 평균값은 D95%3.25±1.7 cGy (RBE), D30%1193.5±10.2 cGy (RBE)의 차이를 보였으며 처방 선량 1%에서의 피부 부피 값 평균은 83.22±4.8% 이내의 차이를 확인하였다. 공기층 두께 변화에 따른 임상표적체적과 피부에서의 선량 모두 큰 변화를 보이지는 않았다. 결론 : 탄소입자 치료를 위해 Solid 형태의 고정기구 제작 시 약간의 공기층은 CTV의 선량 적용 범위를 벗어나지 않는다.

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압연공정을 이용한 가전용 신 바이메탈재의 개발 (Development of New Bimetal Material for Home Appliances by Using the Rolling Process)

  • 박상순;이제헌;배동현;배동수
    • 소성∙가공
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    • 제16권5호통권95호
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    • pp.375-380
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    • 2007
  • The bimetals of home appliances are mainly manufactured by cladding process and these are almost consisted with Cu alloy and Ni alloy. But it is very difficult to clad these alloys, because the brittle $Cu_3O_4$ oxide film formed easily on Cu alloy surface during cladding process. Clad rolling and heat treatment processes were applied for the development of bimetals by using the Ni alloy and the 3 types of Cu alloys. Optical microstructure, micro-hardness, specific resistance, and deflection and line profile of newly processed bimetals specimens were observed and measured in this paper. Inter-diffusion was observed between Cu and Ni element in the interface of heat treated Cu alloy and Ni alloy clad material. The C1220 and Invar36 clad material showed the best property of deflection among the 3 kind of clad materials.

6 DOF 정합을 이용한 대 영역 실리콘 웨이퍼의 3차원 형상, 두께 측정 연구 (3D Surface and Thickness Profile Measurements of Si Wafers by Using 6 DOF Stitching NIR Low Coherence Scanning Interferometry)

  • 박효미;최문성;주기남
    • 한국정밀공학회지
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    • 제34권2호
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    • pp.107-114
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    • 2017
  • In this investigation, we describe a metrological technique for surface and thickness profiles of a silicon (Si) wafer by using a 6 degree of freedom (DOF) stitching method. Low coherence scanning interferometry employing near infrared light, partially transparent to a Si wafer, is adopted to simultaneously measure the surface and thickness profiles of the wafer. For the large field of view, a stitching method of the sub-aperture measurement is added to the measurement system; also, 6 DOF parameters, including the lateral positioning errors and the rotational error, are considered. In the experiment, surface profiles of a double-sided polished wafer with a 100 mm diameter were measured with the sub-aperture of an 18 mm diameter at $10\times10$ locations and the surface profiles of both sides were stitched with the sub-aperture maps. As a result, the nominal thickness of the wafer was $483.2{\mu}m$ and the calculated PV values of both surfaces were $16.57{\mu}m$ and $17.12{\mu}m$, respectively.

수치모델을 이용한 pulsed dc bias ICP장치의 플라즈마 특성 해석 (Numerical Modeling of Plasma Characteristics of ICP System with a Pulsed dc Bias)

  • 주정훈
    • 한국표면공학회지
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    • 제43권3호
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    • pp.154-158
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    • 2010
  • Numerical analysis is done to investigate the effects of pulse bias on the plasma processing characteristics like ion doping and ion nitriding by using fluid dynamic code with a 2D axi-symmetric model. For 10 mTorr of Ar plasma, -1 kV of pulse bias was simulated. Maximum sheath thickness was around 20 mm based on the electric potential profile. The peak electron temperature was about 20 eV, but did not affect the averaged plasma characteristics of the whole chamber. Maximum ion current density incident on the substrate was 200 $A/m^2$ at the center, but was decreased down to 1/10th at radius 100 mm, giving poor radial uniformity.

Numerical Simulation of 3D Free-Surface Flows by Using CIP-based and FV-based Methods

  • Yang, Kyung-Kyu;Nam, Bo-Woo;Kim, Yong-Hwan
    • International Journal of Ocean System Engineering
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    • 제1권3호
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    • pp.136-143
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    • 2011
  • In this paper, three-dimensional free-surface flows are simulated by using two different numerical methods, the constrained interpolation profile (CIP)-based and finite volume (FV)-based methods. In the CIP-based method, the governing equations are solved on stationary staggered Cartesian grids by a finite difference method, and an immersed boundary technique is applied to deal with wave-body interactions. In the FV-based method, the governing equations are solved by applying collocated finite volume discretization, and body-fitted meshes are used. A free-surface boundary is considered as the interface of the multi-phase flow with air and water, and a volumeof-fluid (VOF) approach is applied to trace the free surface. Among many variations of the VOF-type method, the tangent of hyperbola for interface capturing (THINC) and the compressive interface capturing scheme for arbitrary meshes (CICSAM) techniques are used in the CIP-based method and FV-based method, respectively. Numerical simulations have been carried out for dam-breaking and wave-body interaction problems. The computational results of the two methods are compared with experimental data and their differences are observed.