• Title/Summary/Keyword: Liquid Fraction

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Pore Filling Theory of Liquid Phase Sintering and Microstrcture Evolution (액상소결의 기공채움 이론과 미세구조 발달)

  • 이성민
    • Journal of Powder Materials
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    • v.6 no.1
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    • pp.81-87
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    • 1999
  • Based on the pore filling theory, the microstructure evolution during liquid-phase sintering has been analyzed in terms of interrelationship between average grain size and relative density. For constant liquid volume fraction, the microsturucture trajectories reduced to a single curve in a grain size(x)-density(y) map, regardless of grain growth constant. The slope of curves in the map was inversely proportional to average pore size, while it increased fapidly with liquid volume fraction. Increase in pore volume fraction retarded the densification considerably, but showed marginal effect on the slope. The activation energy of densification was predicted to be the same as that of grain growth as long as the liquid volume fraction is constant for any temperature range studied. The present analyses on microstricture evolution may demonstrate the usefulness of pore filling theory and provide a guideline for process optimization of liquid-phase sintering.

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Effects of Density Change and Cooling Rate on Heat Transfer and Thermal Stress During Vertical Solidification Process (수직응고 시스템에서 밀도차와 냉각률이 열전달 및 열응력에 미치는 영향)

  • 황기영;이진호
    • Transactions of the Korean Society of Mechanical Engineers
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    • v.19 no.4
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    • pp.1095-1101
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    • 1995
  • Numerical analysis of vertical solidification process allowing solid-liquid density change is performed by a hybrid method between a winite volume method (FVM) and a finite element method (FEM). The investigation focuses on the influence of solid-liquid density change and cooling rates on the motion of solid-liquid interface, solidified mass fraction, temperatures and thermal stresses in the solid region. Due to the density change of pure aluminium, solid-liquid interface moves more slowly but the solidified mass fraction is larger. The cooling rate of the wall is shown to have a significant influence on the phase change heat transfer and thermal stresses, while the density change has a small influence on the motion of the interface, solidified mass fraction, temperature distributions and thermal stresses. As the cooling rate increases, the thermal stresses become higher at the early stage of a solidification process, but it has small influence on the final stresses as the steady state is reached.

Numerical Analysis of Solidification and Melting Phase Change Using Modified PISO algorithm (수정된 PISO 알고리즘을 이용한 응고 및 융해 현상의 수치해석)

  • Kang K. G;Ryou H. S;Hur N.
    • Journal of computational fluids engineering
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    • v.8 no.3
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    • pp.12-20
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    • 2003
  • A numerical procedure for the calculation of solidification and melting phase change using PISO algorithm is presented. In case of phase change problem, the coupling between velocity/pressure/temperature and liquid fraction is important. The converged temperature and liquid fraction solution which satisfies the energy balance is acquired by applying enthalpy method into inner iteration in matrix solver. And a modified PISO algorithm version is introduced to properly solve the coupling between velocity/pressure/temperature and liquid fraction. A comparison of the proposed procedure with a standard iterative method shows improvement both in terms of computing speed and robustness.

A Study on the Real Quality and Void Fraction of Subcooled Refrigerant Flow (과냉 비등류의 실제건도와 보이드율에 관한 연구)

  • Kim, J.H.;Kim, C.S.;Kim, K.K.;Oh, C.
    • Journal of Advanced Marine Engineering and Technology
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    • v.17 no.2
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    • pp.36-43
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    • 1993
  • Real quality and axial void fraction distribution of subcooled refrigerant flow is very important to predict the heat transfer rate and pressure drop in the design of refrigerating system. In the subcooled boiling region, the liquid bulk temperature is still below the corresponding saturation temperature. But beyond the net vapor generation point, bubble detachment is occured actively from the vapor layer formed on the wall. A reliable method to predict the vapor fraction from the liquid bulk temperature is suggested in this paper. And also the actual quality of the subcooled R-113 flow is calculated in the range of 261-1239kg/$m^2$s mass velocity and 10-30K subcooling.

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Simultaneous Quantitative Determination of Flavone Glycosides in Youngia japonica by High-performance Liquid Chromatography (HPLC에 의한 뽀리뱅이 플라본 배당체 화합물의 동시정량)

  • Nugroho, Agung;Park, Hee-Juhn
    • Korean Journal of Plant Resources
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    • v.25 no.5
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    • pp.640-646
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    • 2012
  • This research was attempted to determine the composition of flavone glycosides (luteolin 7-O-glucoside, luteolin 7-O-glucuronide, linarin) in addition to luteolin simultaneously in aerial part of Youngia japonica (Compositae) by high-performance liquid chromatography. The MeOH extract was further fractionated into the three parts, $CHCl_3$ fraction, EtOAc fraction and BuOH fraction, to investigate the contents of the four flavones in the three fractions. The content of luteolin 7-O-glucuronide (10.07 mg/g) was highest in the MeOH extract among those of the flavones. These four compounds were observed to be less than 1.0 mg/g in $CHCl_3$- and EtOAc fractions but relatively high in BuOH fraction.

Relationship between void fraction and mixing in bubble column flow (기포탑 유동에서의 기포분율과 혼합정도의 상관관계)

  • Zahidul, Islam MD;Lee, Jubeom;Park, Hyungmin
    • Journal of the Korean Society of Visualization
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    • v.15 no.1
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    • pp.41-46
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    • 2017
  • Control of mixing and transport processes are the key areas that can be benefited by understanding the hydrodynamics in gas-liquid two-phase flows. In particular, the enhanced bubble-induced liquid-phase mixing is known to be a function of void fraction distribution, gas phase velocity and so on. To further our insight on the characteristics of the liquid-phase mixing induced by the bubbles, in the present study, we experimentally investigate the mixing performance of a rectangular bubble column while changing the void fraction from 0.006 to 0.075%. A shadowgraphy technique is used to measure the gas-phase properties such as void fraction and size/velocity of bubbles. On the other hand, we use dye visualization with low diffusive buoyant dye to directly measure the level of mixing. Finally, we confirm that the time taken for full mixing scales with the inverse of volume void fraction.

True Sedimentation and Particle Packing Rearrangement during Liquid Phase Sintering

  • Lee, Jong-K.;Xu, Lei;Lu, Shu Zu
    • Proceedings of the Korean Powder Metallurgy Institute Conference
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    • 2006.09a
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    • pp.68-69
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    • 2006
  • When an alloy such as Ni-W is liquid phase sintered, heavy solid W particles sedimentate to the bottom of the container, provided that their volume fraction is less than a critical value. The sintering process evolves typically in two stages, diffusiondriven macrosegregation sedimentation followed by true sedimentation. During macrosegregation sedimentation, the overall solid volume fraction decreases concurrently with elimination of liquid concentration gradient. However, in the second stage of true sedimentation, the average solid volume fraction in the mushy zone increases with time. It is proposed that the true sedimentation results from particle rearrangement for higher packing efficiency.

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Gravity Level Dependency of Gas-Liquid Two-Phase Flow

  • Choi, Bu-Hong
    • Journal of Advanced Marine Engineering and Technology
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    • v.27 no.4
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    • pp.487-493
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    • 2003
  • More reliable design of thermal transport. Power acquisition and thermal management systems requires the through understanding of the flow hydrodynamic. the differences and similarities between the two-phase flow characteristics of two-Phase flow influenced by the gravity levels. The data of flow Patterns, void fraction, frictional pressure drop associated with their characteristics were obtained at $\mu\textrm{g}$. 1g and 2g. Flow patterns and void fraction data obtained at three gravity levels were compared with each other and previous models and correlations.

Experimental Study of the Phase Equilibria for $CO_2$ in Liquified Natural Gas Components at 77-219K

  • Yun, Sang-Kook
    • International Journal of Air-Conditioning and Refrigeration
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    • v.11 no.2
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    • pp.61-66
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    • 2003
  • In order to prevent roll-over and a rapid boil-off of LNG in tanks, the phase equilibria of carbon dioxide in liquefied natural gas components as binary mixtures at cryogenic temperatures have been experimentally measured using Fourier transform infrared spectroscopy in conjunction with a specially designed variable pressure/temperature cryostat cell (pathlength 2 mm; pressures up to 30 bar). Solid carbon dioxide has been found to be comparatively soluble in liquid nitrogen (3.25$\times$${10}^{-6}$ mole fraction), liquid methane (1.04$\times$${10}^{-4}$ mole fraction), liquid ethane (3.1$\times$${10}^{-2}$ mole fraction) and liquid propane (6.11$\times$${10}^{-2}$ mole fraction) at their normal boiling temperatures. The solubilities of carbon dioxide in various cryogens, which increased with increasing temperature, are much lower than those obtained by others using gas chromatography. The differences are attributed to infrared spectroscopy selectively measuring dissolved solute in situ whereas gas chromatography measures microscopic particulate solid in addition to dissolved solute.

A Study on the Bubble Behavior in the Vertical-upward Gas Injection (수직상향 기체주입시 기포거동에 관한 연구)

  • Seo, Dong-Pyo;Oh, Yool-Kwon
    • Proceedings of the KSME Conference
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    • 2003.11a
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    • pp.712-716
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    • 2003
  • In the present study, the gas injection system based on air-water model was designed to investigate the behavior characteristics of bubbles injected into a ladle. The parameters such as gas volume fraction and bubble rise velocity were exprementally measured in a gas-liquid flow region. To measure gas volume fraction, an electo-conductivity probe was used and bubble rise velocity was obtained by a high speed CCD camera. Gas volume fraction was symmetric to the axis of nozzle secured on the bottom of a ladle. The bubble rise velocity was calculated for two different experimental conditions. That is, gas flow conditions were following two case: 1) Q = $0.63{\times}10^{-4}$ $m^{3}/s$, 2) $1.26{\times}10^{-4}$ $m^{3}/s$. As a gas injected into the liquid ladle, the liquid-phase region is circulated by bubbles' behavior. The bubble rise velocity was influenced of the circulation flow of liquid phase. As a result, the bubble rise velocity was appeared higher middle region of ladle than near the nozzle.

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