• 제목/요약/키워드: Phase boundary

검색결과 1,097건 처리시간 0.03초

안티-바운드리 스위칭 디지털 지연고정루프 (An Anti-Boundary Switching Digital Delay-Locked Loop)

  • 윤준섭;김종선
    • 전기전자학회논문지
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    • 제21권4호
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    • pp.416-419
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    • 2017
  • 본 논문에서는 고속 DDR3/DDR4 SDRAM을 위한 새로운 디지털 지연고정루프 (delay-locked loop: DLL)를 제안한다. 제안하는 디지털 DLL은 디지털 지연라인의 boundary switching 문제에 의한 jitter 증가 문제를 제거하기 위하여 위상보간 (phase interpolation) 방식의 파인지연라인 (fine delay line)을 채택하였다. 또한, 제안하는 디지털 DLL은 harmonic lock 문제를 제거하기 위하여 새로운 점진직 검색 (gradual search) 알고리즘을 사용한다. 제안하는 디지털 DLL은 1.1V, 38-nm CMOS DRAM 공정으로 설계되었으며, 0.25-2.0 GHz의 주파수 동작 영역을 가진다. 2.0 GHz에서 1.1 ps의 피크-투-피크 (p-p) 지터를 가지며, 약 13 mW의 전력소모를 가진다.

Numerical Simulation of Erosive Wear on an Impact Sprinkler Nozzle Using a Remeshing Algorithm

  • Xu, Yuncheng;Yan, Haijun
    • International Journal of Fluid Machinery and Systems
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    • 제9권4호
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    • pp.287-299
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    • 2016
  • In China, agricultural irrigation water often contains a lot of suspended sediment which may cause the nozzle wear. In this study, a new numerical simulation combing the Discrete Phase Model and a remeshing algorithm was conducted. The geometric boundary deformation caused by the erosion wear, was considered. The weight loss of the nozzle, the node displacement and the flow field were investigated and discussed. The timestep sensitivity analysis showed that the timestep is very critical in the erosion modeling due to the randomness and the discreteness of the erosion behavior. Based on the simulation results, the major deformation of the boundary wall due to the erosion was found at the corners between outlet portion and contraction portion. Based on this remeshing algorithm, the simulated erosion weight loss of the nozzle is 4.62% less compared with the case without boundary deformation. The boundary deformation changes the pressure and velocity distribution, and eventually changes the sediment distribution inside the nozzle. The average turbulence kinetic energy at the outlet orifice is found to decrease with the erosion time, which is believed to change the nozzle's spray performance eventually.

Numerical Study of Interior Ballistics with Moving Boundary

  • Sung, Hyung-Gun;Park, Sol;Hong, Gi-Cheol;Roh, Tae-Seong;Choi, Dong-Whan
    • 한국추진공학회:학술대회논문집
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    • 한국추진공학회 2008년 영문 학술대회
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    • pp.659-665
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    • 2008
  • The 1-D numerical study of the interior ballistics has been conducted. The unsteady compressible 1-D CFD code using SIMPLER algorithm and QUICK scheme has been developed. The mathematical model of the two-phase flow has been established for the behavior of the interior ballistics. The moving boundary due to the projectile motion as the physical phenomena of the interior ballistics results in the varied control volume. In order to analyze the moving boundary, the numerical codes, which apply the ghost-cell extrapolation method and the Lagrangian method respectively, have been developed. The ghost-cell extrapolation method has been used in the Eulerian coordinate system. The Lagrangian method has been used in Non-Eulerian coordinate system. These codes have been verified through the analysis of the free piston motion problem in the tube. Through this study, the basic techniques of the numerical code for the multi-dimensional two-phase flow of the interior ballistics have been obtained.

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PHASE FIELD MODELING OF CRYSTAL GROWTH

  • Sekerka, Robert F.
    • 한국결정성장학회:학술대회논문집
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    • 한국결정성장학회 1996년도 The 9th KACG Technical Annual Meeting and the 3rd Korea-Japan EMGS (Electronic Materials Growth Symposium)
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    • pp.139-156
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    • 1996
  • The phase field model is becoming the model of choice for the theoretical study of the morphologies of crystals growth from the melt. This model provides an alternative approach to the solution of the classical (sharp interface) model of solidification by introducing a new variable, the phase field, Ø, to identify the phase. The variable Ø takes on constant values in the bulk phases and makes a continuous transition between these values over a thin transition layer that plays the role of the classically sharp interface. This results in Ø being governed by a new partial differential equation(in addition to the PDE's that govern the classical fields, such as temperature and composition) that guarantees (in the asymptotic limit of a suitably thin transition layer) that the appropriate boundary conditions at the crystal-melt interface are satisfied. Thus, one can proceed to solve coupled PDE's without the necessity of explicitly tracking the interface (free boundary) that would be necessary to solve the classical (sharp interface) model. Recent advances in supercomputing and algorithms now enable generation of interesting and valuable results that display most of the fundamental solidification phenomena and processes that are observed experimentally. These include morphological instability, solute trapping, cellular growth, dendritic growth (with anisotropic sidebranching, tip splitting, and coupling to periodic forcing), coarsening, recalescence, eutectic growth, faceting, and texture development. This talk will focus on the fundamental basis of the phase field model in terms of irreversible thermodynamics as well as it computational limitations and prognosis for future improvement. This work is supported by the National Science Foundation under grant DMR 9211276

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New Characterization Methods for Block Copolymers and their Phase Behaviors

  • Park, Hae-Woong;Jung, Ju-Eun;Chang, Tai-Hyun
    • Macromolecular Research
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    • 제17권6호
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    • pp.365-377
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    • 2009
  • In this feature article, we briefly review the new methods we have utilized recently in the investigation of morphology and phase behavior of block copolymers. We first describe the chromatographic fractionation method to purify block copolymers from their side products of mainly homopolymers or block copolymer precursors inadvertently terminated upon addition of the next monomer in the sequential anionic polymerization. The chromatographic method is extended to the fractionation of the individual block of diblock copolymers which can yield the diblock copolymer fractions of different composition and molecular weight, which also have narrower distributions in both molecular weight and composition. A more detailed phase diagram could be constructed from the set of block copolymer fractions without the need of acquiring many block copolymers each prepared by anionic polymerization. The fractions with narrow distribution in both molecular weight and composition exhibit better long-range ordering and sharper phase transition. Next, epitaxial relationships between two ordered structures in block copolymer thin film is discussed. We employed the direct visualization method, transmission electron microtomography(TEMT) to scrutinize the grain boundary structure.

$\gamma$-TiAl 합금의 고온변형 및 Cavity 형성 연구 (A Study on the High Temperature Deformation and the Cavity Initiation of Gamma TiAl Alloy)

  • 김정한;하태권;장영원;이종수
    • 한국소성가공학회:학술대회논문집
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    • 한국소성가공학회 2001년도 춘계학술대회 논문집
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    • pp.172-175
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    • 2001
  • The high temperature deformation behavior of two-phase gamma TiAl alloy has been investigated with the variation of temperature and ${\gamma}/{\alpha}_2$ volume fraction. For this purpose, a series of load relaxation tests and tensile tests have been conducted at temperature ranging from 800 to $1050^{\circ}C$. In the early stage of the deformation as in the load relaxation test experimental flow curves of the fine-grained TiAl alloy are well fitted with the combined curves of two processes (grain matrix deformation and dislocation climb) in the inelastic deformation theory. The evidence of grain boundary sliding has not been observed at this stage. However, when the amount of deformation is large (${\epsilon}{\approx}$ 0.8), flow curves significantly changes its shape indicating that grain boundary sliding also operates at this stage, which has been attributed to the occurrence of dynamic recrystallization during the deformation. With the increase in the volume fraction of ${\alpha}_2$-phase, the flow stress for grain matrix deformation increases since ${\alpha}_2$-Phase is considered as hard phase acting as barrier for dislocation movement. It is considered that cavity initiation is more probable to occur at ${\alpha}_2/{\gamma}$ interface rather than at ${\gamma}/{\gamma}$ interface.

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오일러 격자체계에서 유체율 함수에 기초한 경계면 추적기법의 비교 (Comparison of Volume of Fluid (VOF) type Interface Capturing Schemes using Eulerian Grid System)

  • 김도삼;김탁겸;신범식;이광호
    • 한국해안·해양공학회논문집
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    • 제32권1호
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    • pp.1-10
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    • 2020
  • 자유수면을 포함하는 파동장과 같이 단상의 경계가 시간발전에 따라 지속적으로 변화하는 경우나 액상과 기상이 혼합되는 문제에 있어서는 다상유동(multiphase flow) 문제를 적용하는 예가 증가하고 있다. 특히, 파동장과 같은 자유수면의 문제를 취급하는데 있어서는 혼합되지 않는 액상과 기상의 비압축성 뉴턴유체를 고려한 혼상류 모델이 적용되는 경우가 많다. 일반적으로 혼상류 모델은 각상의 경계면에 대한 시간기반 거동추적이 필수적이며, 궁극적으로는 계산의 정도를 좌우한다. 본 연구는 다양한 CFD 수치해석코드에 적용되고 있는 대표적인 VOF-type의 경계면 추적기법들의 이류성능을 평가하였다. 특히, 기존의 전통적인 VOF-type의 경계면 추적기법 및 이류계산에서 발생하는 수치확산을 최소화하기 위해 수치유속(numerical flux)을 제어하는 FCT 법의 효용성을 평가하고, 더불어 CIP 법을 활용한 자유수면 추적성능의 가능성을 고찰하였다. 그 결과, 본 연구에서 적용한 제한된 조건하에서는 수치확산 방지를 위해 수치확산방지 유속을 도입한 FCT-VOF 법이 가장 높은 경계면의 추적성능을 보였다. 본 연구에서 도출되는 결과는 다양한 수치해석코드에 적용되는 자유수면의 추적기법을 선택함에 있어서 중요한 기초자료로 활용될 것으로 기대된다.

ZnO-Co3O4-Cr2O3-La2O3 세라믹스의 결함과 입계 특성에 미치는 CaCO3의 영향 (Effects of CaCO3 on the Defects and Grain Boundary Properties of ZnO-Co3O4-Cr2O3-La2O3 Ceramics)

  • 홍연우;하만진;백종후;조정호;정영훈;윤지선
    • 한국전기전자재료학회논문지
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    • 제31권5호
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    • pp.307-312
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    • 2018
  • Liquid phases in ZnO varistors cause more complex phase development and microstructure, which makes the control of electrical properties and reliability more difficult. Therefore, we have investigated 2 mol% $CaCO_3$ doped $ZnO-Co_3O_4-Cr_2O_3-La_2O_3$ (ZCCLCa) bulk ceramics as one of the compositions without liquid phase sintering additive. The results were as follows: when $CaCO_3$ is added to ZCCLCa ($644{\Omega}cm$) acting as a simple ohmic resistor, CaO does not form a secondary phase with ZnO but is mostly distributed in the grain boundary and has excellent varistor characteristics (high nonlinear coefficient ${\alpha}=78$, low leakage current of $0.06{\mu}A/cm^2$, and high insulation resistance of $1{\times}10^{11}{\Omega}cm$). The main defects $Zn_i^{{\cdot}{\cdot}}$ (AS: 0.16 eV, IS & MS: 0.20 eV) and $V_o^{\bullet}$ (AS: 0.29 eV, IS & MS: 0.37 eV) were found, and the grain boundaries had 1.1 eV with electrically single grain boundary. The resistance of each defect and grain boundary decreases exponentially with increasing the measurement temperature. However, the capacitance (0.2 nF) of the grain boundary was ~1/10 lower than that of the two defects (~3.8 nF, ~2.2 nF) and showed a tendency to decrease as the measurement temperature increased. Therefore, ZCCLCa varistors have high sintering temperature of $1,200^{\circ}C$ due to lack of liquid phase additives, but excellent varistor characteristics are exhibited, which means ZCCLCa is a good candidate for realizing chip type or disc type commercial varistor products with excellent performance.

고온-고압하에서 티탄철석에 대한 상면이 연구 (Phase Transition Study on Ilmenite under High Pressure and Temperature)

  • Kim, Young-Ho
    • 한국광물학회지
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    • 제15권3호
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    • pp.161-169
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    • 2002
  • 고온-고압 상태에서 티탄철석 ($FeTiO_3$)의 상변이에 대한 연구가 있었으나, 그 결과는 서로 일치하지 않고 있다. 특히, 티탄철석상과 페롭스카이트상의 상변이 경계는 담금방법에 의해 결정된 것으로 신뢰도에 의문이 제기되고 있다. 이러한 문제를 해결하기 위해, 고온-고압 현장상태에서 라지 볼륨 기기와 방사광을 이용하여 19 GPa와 $700^{\circ}C$의 범위에서 X선 회절실험을 시행하였다. 이러한 실험결과, 페롭스카이트상은 상온에서 16 CPa 이상의 압력에서 안정하며, 15 CPa 근처에서 $LiNbO_3$상으로 변이한다. 또한 이 두 고온-고압상은 $500^{\circ}C$에서는 순간적인 상변이를 하고 있다. $LiNbO_3$상은 각각 13 CPa 및 300'E와 10.8 GPa 및 400'E에서 티탄철석상으로 상변이 한다. 따라서 본 실험결과는 $LiNbO_3$상은 고온-고압하에서 안정 영역을 확보하고 있으며, 페롭스카이트-티탄철석상경계는 이전에 발표된 결과와는 매우 다르다는 것을 지시해주고 있다.

고크롬 (α+γ) 2상강의 결정립 성장기구 (A study on the grain growth mechanism in dual-phase high Cr-steel)

  • 위명용
    • 열처리공학회지
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    • 제11권4호
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    • pp.324-332
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    • 1998
  • The grain growth characteristics of dual-phase (${\alpha}+{\gamma}$) containing high Cr-steel have investigate using ${\alpha}$-, ${\gamma}$-single phases and (${\alpha}+{\gamma}$)dual-phase of 12%Cr Steel. The heat treatment has performed at $1000-1200^{\circ}C$ for 1-100hr. The results are as follows : 1) The grain growth rate in (${\alpha}+{\gamma}$) dual phase was substantially slower than that of single grain. 2) The relation between mean grain radius $\bar{{\gamma}}$ and annealing time t is, in general, described as following equation : $$(\bar{{\gamma}})^n-(\bar{{\gamma}_o})^n=K_n{\cdot}t{\cdots}{\cdots}(1)$$ i) In the case of single phase of high Cr steel, Eq.(1) is described as $(\bar{{\gamma}})^2-(\bar{{\gamma}_o})^2=K_2{\cdot}t$ and the grain growth is controlled by boundary migration. ii) In dual phase, the grain growth needs diffusion of alloying elements because the chemical composition of ${\alpha}$- and ${\gamma}$- phases differs from each other. When the volume fraction of ${\alpha}$-, ${\gamma}$-phase was almost equal and ${\gamma}$-phase in the case of 80 and $90%{\gamma}$. Eq.(1) is described as $(\bar{{\gamma}})^3-(\bar{{\gamma}_o})^3=K_3{\cdot}t$ because the grain growth is controlled by volume diffusion iii) In the case of ${\gamma}$-rich phase (80 and $90%{\gamma}$), the grain growth of minor phase (10 and $20%{\alpha}$) is described as $(\bar{{\gamma}})^4-(\bar{{\gamma}_o})^4=K_4{\cdot}t$ because the boundary diffusion is predominent rather than volume diffusion.

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