17 research outputs found

    Development of accurate and efficient numerical methods for bubble-particle interaction

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    DoctorAccurate and efficient numerical methods have been developed to simulate flow including bubble-particle interaction. First, to achieve high scalability for large computation, the Navier-Stokes equations are solved by an alternating-directional- implicit (ADI) method parallelized by a parallel diagonal dominant (PDD) algorithm. Second, the phase interface is tracked by a conservative volume-of-fluid (VOF) method. The developed numerical methods have been further improved by modeling bubble-particle interaction. New algorithms are proposed to predict that particles are attached or slide away on the bubble surface in a VOF framework. Fluid motions are predicted in an Eulerian frame, while particle motions are predicted in a Lagrangian framework. To consider bubble-particle interaction, numerical models connecting phase interfaces and solid particles are required. In this study, algorithms that are used to detect collision and determine the sliding or attachment of the particle are developed. An effective bubble is also introduced to model the bubble-particle interaction in a VOF framework. The proposed numerical method is validated through experimental cases that entail the rising of a single bubble with particles. Collision and attachment probabilities obtained from the simulation are compared to theoretical and experimental results based on bubble diameters, particle diameters, and contact angles. The particle trajectories near the bubble are presented to show differences with and without the proposed bubble-particle interaction model. The sliding and attachment of the colliding particle are observed using this model

    A Case study of sport education curriculum model in teaching physical education at a selected secondary school

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :์ฒด์œก๊ต์œก๊ณผ,1998.Docto

    Effect of Zr on Liquid-Liquid Phase Separation in Microstructure of Cu-Fe alloys

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    Master๋™์ฒ ํ•ฉ๊ธˆ์˜ ํ˜ผํ•ฉ ์—”ํƒˆํ”ผ๋Š” ์–‘์˜ ๊ฐ’์„ ๊ฐ–์œผ๋ฉฐ ๋Œ€ํ‘œ์ ์ธ ์ƒ๋ถ„๋ฆฌ ํ•ฉ๊ธˆ์œผ๋กœ ์•Œ๋ ค์ ธ ์žˆ์œผ๋ฉฐ, ์€ ์˜จ๋„ ๊ตฌ๊ฐ„์˜ ๊ณ ์•ก ๊ณต์กด ์˜์—ญ์ด ์กด์žฌํ•˜์—ฌ ํ•˜๋‚˜์˜ ์•ก์ƒ์ด ๋‘ ๊ฐœ์˜ ์•ก์ƒ ์œผ๋กœ ๋‚˜๋ˆ„์–ด์ง€๋Š” ์•ก์ƒ๋ถ„๋ฆฌ ๊ฑฐ๋™์ด ๋ฐœ์ƒํ•œ๋‹ค. ์ด ๊ฑฐ๋™์„ ์ œ์–ดํ•˜๊ธฐ ์œ„ํ•œ ๋งŽ์€ ์‹œ๋„๊ฐ€ ์žˆ์—ˆ์ง€๋งŒ ๋šœ๋ ทํ•œ ๊ฒฐ๊ณผ๋Š” ์ง€๊ธˆ๊นŒ์ง€ ๋ฐœ๊ฒฌ๋˜์ง€ ์•Š์•˜๋‹ค. Zr์„ ๋™์ฒ ํ•ฉ๊ธˆ์— ์ฒจ๊ฐ€ํ•จ์œผ๋กœ ์„œ ๋‹ฌ๋ผ์ง€๋Š” ๊ฒƒ์€ ์ฒซ ๋ฒˆ์งธ, ํ˜ผํ•ฉ ์—”ํƒˆํ”ผ ๊ฐ’์„ ๋‚ฎ์ถ”๊ณ  ๋™์‹œ์— ํ˜ผํ•ฉ ์—”ํŠธ๋กœํ”ผ๋ฅผ ์ฆ๊ฐ€์‹œ ํ‚ด์œผ๋กœ์จ ํ˜ผํ•ฉ ๊น์Šค ์ž์œ  ์—๋„ˆ์ง€ ๊ฐ’์ด ํฌ๊ฒŒ ๋‚ฎ์•„์ง€๊ฒŒ ๋˜๋Š” ๊ฒƒ์ด๋‹ค. ๋‘ ๋ฒˆ์งธ๋Š” ์‹คํ—˜ ๊ณผ์ • ์ค‘์— Zr์ด ์‚ฐ์†Œ์™€ ๋ฐ˜์‘ํ•˜์—ฌ ZrO2๊ฐ€ ๋˜๋ฉด ์ด๋Š” ฮณ-Fe๊ณผ ์ ์€ lattice mismatch ๋กœ ์ธํ•ด์„œ ๊ท ์ผ ํ•ต์ƒ์„ฑ์„ ๋•๋Š” ์—ญํ• ์„ ํ•˜๊ฒŒ ๋œ๋‹ค. ๋งˆ์ง€๋ง‰์œผ๋กœ๋Š” ๊ธˆ์†๊ฐ„ ํ™”ํ•ฉ๋ฌผ์ด ํ˜•์„ฑ๋˜์ง€๋งŒ ์ด๋Š” ์•ก์ƒ๋ถ„๋ฆฌ ๊ฑฐ๋™์—๋Š” ์˜ํ–ฅ์„ ๋ฏธ์น˜์ง€ ์•Š์Œ์„ ํ™•์ธํ•˜์˜€๋‹ค. ๊ธฐ์กด ๋™์ฒ  ํ•ฉ๊ธˆ์˜ ์‘๊ณ  ์ˆœ์„œ๋Š” ์•ก์ƒ๋ถ„๋ฆฌ๊ฐ€ ์ผ์–ด๋‚œ ํ›„ ํฐ ๊ณผ๋ƒ‰๋„์™€ ํ•จ๊ป˜ Binodal curve ๋‚ด์—์„œ ฮณ-Fe์˜ ํ•ต์ƒ์„ฑ์ด ์‹œ์ž‘๋˜๋Š” ๋ฐ˜๋ฉด์—, Zr์ด ์ฒจ๊ฐ€๋œ ๋™์ฒ ํ•ฉ๊ธˆ์€ ์•ก์ƒ์„ ๊ณผ Binodal curve ์‚ฌ์ด์—์„œ ์•ก์ƒ๋ถ„๋ฆฌ๊ฐ€ ์ผ์–ด๋‚˜์ง€ ์•Š๊ณ  ์ ์€ ๊ณผ๋ƒ‰์œผ๋กœ ฮณ-Fe์˜ ํ•ต์ƒ์„ฑ์ด ์‹œ์ž‘ํ•˜๋Š” ๊ฒƒ์„ ์‹œ์ฐจ ์ฃผ์‚ฌ ์—ด๋Ÿ‰๊ณ„ (DSC)๋ฅผ ํ†ตํ•ด์„œ ๋ฐํ˜€๋ƒˆ๋‹ค. ๋˜ํ•œ, Zr ์ฒจ๊ฐ€์˜ ์˜ํ–ฅ์œผ๋กœ ๋ณ€ํ•˜๋Š” DSC ์˜ ๋ฐœ์—ด ๊ทธ๋ž˜ํ”„๋ฅผ ํ†ตํ•ด ๊ฒฐ์ •ํ™”๋„๋ฅผ ๊ณ„์‚ฐํ•จ์œผ๋กœ์จ ์ˆ˜์ง€์ƒ์ •์€ ๋น„๊ต์  ์ ์ง€๋งŒ ์กฐ๋Œ€ํ•œ ๊ฒƒ์„ ์•Œ ์ˆ˜ ์žˆ๋‹ค. ZrO2์˜ ์ง์ ‘์ ์ธ ์กด์žฌ์™€ ์—ญํ• ์„ ๋ฐœ๊ฒฌํ•˜์ง„ ๋ชปํ•˜์˜€์œผ๋‚˜ ๊ณ ์ „ ํ•ต์ƒ์„ฑ ์ด๋ก ์„ ํ†ตํ•ด ํ•ต์ƒ์„ฑ ์†๋„๋ฅผ ๊ณ„์‚ฐํ•˜๋Š” ๊ฒƒ์œผ๋กœ Zr์ด ์ฒจ๊ฐ€๋œ ๋™์ฒ ํ•ฉ๊ธˆ์—์„œ ๊ท ์ผ ํ•ต์ƒ์„ฑ์„ ์ด‰์ง„ ๋œ๋‹ค๋Š” ์ฆ๊ฑฐ๋ฅผ ํ†ตํ•ด ZrO2๊ฐ€ ์กด์žฌํ•  ์ˆ˜ ๋ฐ–์— ์—†์Œ์„ ๊ฐ„์ ‘์ ์œผ๋กœ ์ฆ๋ช…ํ•˜์˜€๋‹ค. ๊ฒฐ๊ณผ์ ์œผ๋กœ, ๋™์ฒ ํ•ฉ๊ธˆ์˜ ์•ก์ƒ๋ถ„๋ฆฌ ๊ฑฐ๋™์€ Zr์ด ์ฒจ๊ฐ€๋จ์œผ๋กœ์„œ ๋ช…๋ฐฑํžˆ ์ œ์–ด๋จ์„ ๋ณด์ธ๋‹ค.In the Cu-Fe binary phase diagram, the metastable miscibility gap exists in the liquid-solid coexisting zone. Assuming that ฮณ-Fe nucleation has occurred between the liquidus line and the binodal curve with low supercooling, it could be obtained fully dendritic microstructure and there is no liquid-liquid phase separation (LLPS) behavior throughout the specimens. But, ฮณ-Fe nucleation started under binodal curve with high supercooling, LLPS behavior was investigated and minority phase droplets were obtained in the microstructure of CFA. The LLPS behavior was possible to control by promoting ฮณ-Fe nucleation that happened above the binodal curve. For a combination of classical nucleation theory and thermal instrumental analysis, Zr is added to CFA to decrease the Gibbs free energy of mixing and form ZrO2 that accelerates heterogeneous nucleation by acting as a nucleation site for ฮณ-Fe. Furthermore, to observe clear evidence of LLPS behavior and ฮณ-Fe crystallization by adding 1wt๏ผ…Zr to Cu-40wt๏ผ…Fe and Cu-20wt๏ผ…Fe respectivel

    Computational Analysis of an Air Jet in Cross Water Flow

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