4 research outputs found

    ๋‹ค์–‘ํ•œ ์—ด์œ ๋™๋ถ€ํ•˜ ์‹œ์Šคํ…œ์˜ ๋ฐ˜์‘์œ ๋™ ๋ฐ ๊ตฌ์กฐ ์ƒํ˜ธ์ž‘์šฉ ํ•ด์„์„ ์œ„ํ•œ 3์ฐจ์› ์ฝ”๋“œ ๊ฐœ๋ฐœ ์—ฐ๊ตฌ

    Get PDF
    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€, 2019. 2. ์—ฌ์žฌ์ต.Previously researched fluid-structure interaction analysis has mostly simulated an interaction between a structure and non-reactive flow, which does not consider the chemical reaction in flow. In the interaction analysis of large deformation of a structure due to high temperature and pressure flow accompanied by chemical reactions such as explosion or combustion, it is difficult to apply the geometry of the deformed structure to the fluid flow domain. In this reason, many studies have not been conducted to simultaneously analyze the interaction between the reactive flow and the structure deformation. Instead, the temperature and pressure conditions of the flow field analyzed in the body are applied to the boundary conditions of the structure analysis. In this case, the flow could not be interpreted according to the behavior of the structure, so the exact pressure and temperature near the structure could not be calculated. In this study, a three-dimensional simulation techniques were developed for analyze the reactive flow including the chemical reaction with the large deformation of structure. The numerical code is verified by comparing the simulation results with the experimental values. In this study, various reactive flows were considered. The ethylene-air mixture and the kerosene-air mixture, which are gaseous high energy materials, simulate the combustion reaction through the 1-step Arrhenius equation. In addition, combustion characteristics of anisotropic PETN and HMX, which are solid energetic materials, were analyzed by using the modified anisotropic I&G model. The developed combustion model compared the C-J condition and the detonation cell size. Structure deformation was performed by using Eulerian or Lagrangian analysis method and the method was verified by comparing with the experimental data of Taylor impact problem. A level set technique and a ghost fluid method (GFM) were used to set boundary values and trace the interface between the reactive flow and the structure. In order to verify the multi-material analysis method, the cantilever motion in the flow field and the tube deformation problem due to detonation load were simulated. The numerical results are verified by comparing with the theoretical and experimental values. For the three dimensional simulation, the STL file to level converting algorithm was developed. Moreover, the adaptive mesh refinement (AMR) and message passing interface (MPI) for parallel processing were conducted to reduce the computation time and resources. The interactions between reactive flow and structure under various thermal hydrodynamic loading systems were analyzed based by developed code. The behavior of rear cover which is deformed by the launching rocket plume inside a vertical launching system (VLS) is analyzed. This analysis results were verified by comparing with the experimental data, and the influence of rear cover deformation on the flow was confirmed through the analysis results. In addition, the explosion of the solid explosives in the three-dimensional concrete building, which cannot be simplified in two dimensions, and the pressure transmitted to the wall are analyzed. The numerical analysis results were compared with experimental data. In the analysis of tube deformation due to detonation inside the metal tube was simulated. The yield stress of metal tube is dependent on wall temperature and thermal softening was considered. In case of pulse detonation engine (PDE), which is exposed to high temperature environment, accurate results can be obtained by using temperature dependent properties and simulation results verified by comparison with theoretical failure model. The elastically vibrating tube was considered for detonation inside the PDE simulation. Due to the repetitively detonation propagation inside PDE, the PDE wall is vibrated with its natural frequency even if the PDE does not be destroyed. The simulation results confirms that propagation of detonation is affected by the deformation of tube.๊ธฐ์กด์— ์ˆ˜ํ–‰๋˜์–ด์˜จ ์œ ์ฒด-๊ตฌ์กฐ ์—ฐ์„ฑ ํ•ด์„์€ ๋Œ€๋ถ€๋ถ„ ์œ ๋™์˜ ํ™”ํ•™ ๋ฐ˜์‘์„ ๊ณ ๋ คํ•˜์ง€ ์•Š๋Š” ๋น„๋ฐ˜์‘์„ฑ ์œ ๋™๊ณผ ๊ตฌ์กฐ์ฒด์˜ ์ƒํ˜ธ์ž‘์šฉ์„ ํ•ด์„ํ•ด ์™”๋‹ค. ์ด๋Š” ํญ๋ฐœ์ด๋‚˜ ์—ฐ์†Œ ๊ฐ™์€ ํ™”ํ•™๋ฐ˜์‘์„ ๋™๋ฐ˜ํ•˜๋Š” ๊ณ ์˜จ, ๊ณ ์••์˜ ์œ ๋™๊ณผ ๊ตฌ์กฐ์˜ ์—ฐ์„ฑ ํ•ด์„ ์‹œ์— ๊ตฌ์กฐ์ฒด์˜ ๋Œ€๋ณ€ํ˜•์ด ์ผ์–ด๋‚˜๊ธฐ ๋•Œ๋ฌธ์ด๋‹ค. ๊ธฐ์กด์˜ ์œ ์ฒด-๊ตฌ์กฐ ์—ฐ์„ฑ ํ•ด์„ ๊ธฐ๋ฒ•์œผ๋กœ ๊ธ‰๊ฒฉํ•˜๊ฒŒ ๋ณ€ํ˜•๋˜๋Š” ๊ตฌ์กฐ์˜ ํ˜•์ƒ์„ ์ฆ‰๊ฐ์ ์œผ๋กœ ์œ ๋™์žฅ์— ์ ์šฉํ•˜๋Š”๋ฐ ๋งค์šฐ ๋งŽ์€ ๊ณ„์‚ฐ ์‹œ๊ฐ„๊ณผ ์˜ค์ฐจ๊ฐ€ ์žˆ๊ธฐ ๋•Œ๋ฌธ์— ๋ฐ˜์‘์„ฑ ์œ ๋™๊ณผ ๊ตฌ์กฐ์˜ ์ƒํ˜ธ์ž‘์šฉ์„ ๋™์‹œ์— ํ•ด์„ํ•˜๋Š” ์—ฐ๊ตฌ๋Š” ๋งŽ์ด ์ˆ˜ํ–‰๋˜์ง€ ์•Š์•˜๋‹ค. ๋”ฐ๋ผ์„œ ๊ธฐ์กด ์—ฐ๊ตฌ์—์„œ๋Š” ๊ณ ์ •๋œ ๊ตฌ์กฐ์ฒด์—์„œ ํ•ด์„๋œ ํ™”ํ•™๋ฐ˜์‘์„ ํฌํ•จํ•œ ์œ ๋™์˜ ์˜จ๋„์™€ ์••๋ ฅ์„ ๊ตฌ์กฐ ํ•ด์„์— ์ ์šฉํ•˜๋Š” ๋ฐฉ๋ฒ•์œผ๋กœ ์œ ์ฒด-๊ณ ์ฒด ์—ฐ์„ฑ ํ•ด์„์„ ์ œํ•œ์ ์œผ๋กœ ์ˆ˜ํ–‰ํ•˜์˜€๋‹ค. ์ด ๊ฒฝ์šฐ, ๊ตฌ์กฐ์˜ ๊ฑฐ๋™์— ๋”ฐ๋ผ ๋ฐ”๋€Œ๋Š” ์œ ๋™์„ ํ•ด์„ํ•˜์ง€ ๋ชปํ•˜๋ฏ€๋กœ ๊ตฌ์กฐ์— ์ „๋‹ฌ๋˜๋Š” ์ •ํ™•ํ•œ ์••๋ ฅ ๋ฐ ์˜จ๋„ ์กฐ๊ฑด์„ ๋ฐ˜์˜ํ•  ์ˆ˜ ์—†๋‹ค. ํŠนํžˆ 3์ฐจ์›์˜ ๋ณต์žกํ•œ ํ˜•์ƒ์—์„œ๋Š” ๊ตฌ์กฐ ๋ณ€ํ˜•์„ ์œ ๋™ ํ•ด์„์— ์ ์šฉํ•˜๊ธฐ ๋งค์šฐ ์–ด๋ ต๊ธฐ ๋•Œ๋ฌธ์— 3์ฐจ์›์˜ ๋ฐ˜์‘์„ฑ ์œ ๋™๊ณผ ๊ตฌ์กฐ์˜ ์—ฐ์„ฑ ์—ฐ๊ตฌ๋Š” ๊ฑฐ์˜ ์ˆ˜ํ–‰๋˜์ง€ ์•Š์•˜๋‹ค. ๋”ฐ๋ผ์„œ ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ํ™”ํ•™๋ฐ˜์‘์„ ํฌํ•จํ•˜๋Š” ๋ฐ˜์‘์„ฑ ์œ ๋™๊ณผ ์ด์— ๋”ฐ๋ฅด๋Š” ๊ตฌ์กฐ์ฒด์˜ ๋Œ€๋ณ€ํ˜•์„ ํ•จ๊ป˜ ํ•ด์„ํ•  ์ˆ˜ ์žˆ๋Š” ๊ธฐ๋ฒ•์„ ๊ฐœ๋ฐœํ•˜์˜€๊ณ  ์ด๋ฅผ 3์ฐจ์›์— ํ™•์žฅ์‹œํ‚ค๊ธฐ ์œ„ํ•˜์—ฌ ๋‹ค์–‘ํ•œ ์ˆ˜์น˜์  ๊ธฐ๋ฒ•๋“ค์„ ๊ฐœ๋ฐœํ•˜๊ณ  ์ ์šฉํ•˜์˜€๋‹ค. ๊ฐœ๋ฐœ๋œ ํ•ด์„ ๊ธฐ๋ฒ•์€ ์‹คํ—˜ ๊ฐ’๊ณผ ๋น„๊ตํ•˜์—ฌ ๊ทธ ํƒ€๋‹น์„ฑ์„ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ๋‹ค์–‘ํ•œ ๋ฐ˜์‘์„ฑ ์œ ๋™์„ ๊ณ ๋ คํ•˜์˜€๋‹ค. ๊ธฐ์ฒด ๊ณ ์—๋„ˆ์ง€ ๋ฌผ์งˆ์ธ ์—ํ‹ธ๋ Œ-๊ณต๊ธฐ ํ˜ผํ•ฉ๋ฌผ, ์ผ€๋กœ์‹ -๊ณต๊ธฐ ํ˜ผํ•ฉ๋ฌผ ๋ฟ๋งŒ ์•„๋‹ˆ๋ผ ๊ณ ์ฒด ๊ณ ์—๋„ˆ์ง€ ๋ฌผ์งˆ์ธ ์ด๋ฐฉ์„ฑ PETN๊ณผ HMX์˜ ์—ฐ์†Œ ๋ฐ˜์‘ ๋ชจ๋ธ์„ ์ œ์‹œํ•˜์˜€๋‹ค. ๊ธฐ์ฒด์˜ ๊ฒฝ์šฐ 1๋‹จ๊ณ„ ์•„๋ ˆ๋‹ˆ์šฐ์Šค์‹์„ ํ†ตํ•˜์—ฌ ์—ฐ์†Œ๋ฐ˜์‘์„ ๋ชจ์‚ฌํ•˜์˜€๊ณ , ๊ณ ์ฒด์˜ ๊ฒฝ์šฐ ๋ณ€ํ˜•๋œ ์ด๋ฐฉ์„ฑ I&G ๋ชจ๋ธ์„ ์‚ฌ์šฉํ•˜์—ฌ ์ถฉ๊ฒฉ ๋ฐฉํ–ฅ์— ๋”ฐ๋ฅธ ์—ฐ์†Œ ํŠน์„ฑ์„ ํ•ด์„ํ•˜์˜€๋‹ค. ๊ฐœ๋ฐœ๋œ ์—ฐ์†Œ ๋ชจ๋ธ์€ C-J ์กฐ๊ฑด ๋ฐ ๋ฐํ† ๋„ค์ด์…˜ ์…€ ํฌ๊ธฐ๋ฅผ ๋น„๊ต ๊ฒ€์ฆ ํ•˜์˜€๋‹ค. ๊ตฌ์กฐ์ฒด ๋ณ€ํ˜•์€ ์˜ค์ผ๋Ÿฌ๋ฆฌ์•ˆ๊ณผ ๋ผ๊ทธ๋ž‘์ง€์•ˆ์˜ ๊ธฐ๋ฐ˜์˜ ๊ตฌ์กฐ ํ•ด์„ ๋ฐฉ์‹์„ ์‚ฌ์šฉํ•˜์—ฌ ์ •ํ™•ํ•œ ๊ตฌ์กฐํ•ด์„์„ ์ˆ˜ํ–‰ํ•˜์˜€์œผ๋ฉฐ ํ…Œ์ผ๋Ÿฌ ์ถฉ๊ฒฉ๋ฌธ์ œ๋ฅผ ์‹คํ—˜๊ฐ’๊ณผ ๋น„๊ตํ•˜์—ฌ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ๋ฐ˜์‘์„ฑ ์œ ๋™๊ณผ ๊ตฌ์กฐ์ฒด์˜ ๊ฒฝ๊ณ„๋ฉด ์ถ”์ ๊ณผ ๊ฒฝ๊ณ„๊ฐ’ ์„ค์ •์„ ์œ„ํ•˜์—ฌ ๊ฐ๊ฐ ๋ ˆ๋ฒจ์…‹ ๊ธฐ๋ฒ•๊ณผ ๊ฐ€์ƒ์œ ์ฒด๊ธฐ๋ฒ•์„ ํ™œ์šฉํ•˜์˜€๋‹ค. ๋‹ค๋ฌผ์งˆ ํ•ด์„์˜ ์ ์ ˆ์„ฑ์„ ๊ฒ€์ฆํ•˜๊ธฐ ์œ„ํ•˜์—ฌ, ์œ ๋™์žฅ ๋‚ด์—์„œ์˜ ์™ธํŒ”๋ณด์˜ ์›€์ง์ž„๊ณผ ๋ฐํ† ๋„ค์ด์…˜ ํ•˜์ค‘์— ์˜ํ•œ ๊ด€ ๋ณ€ํ˜• ๋ฌธ์ œ๋ฅผ ์ด๋ก ๊ฐ’ ๋ฐ ์‹คํ—˜๊ฐ’๊ณผ ๋น„๊ตํ•˜์—ฌ ๊ฒ€์ฆํ•˜์˜€๋‹ค. 3์ฐจ์›์—์„œ์˜ ํ•ด์„์„ ์œ„ํ•˜์—ฌ STL ํŒŒ์ผ์„ ๋ ˆ๋ฒจ๋กœ ๋ณ€ํ™˜ํ•˜๋Š” ์•Œ๊ณ ๋ฆฌ์ฆ˜์„ ๊ฐœ๋ฐœ ํ•˜์˜€์œผ๋ฉฐ ๊ณ„์‚ฐ ์‹œ๊ฐ„ ๋‹จ์ถ•์„ ์œ„ํ•˜์—ฌ ์ ์‘์  ๊ฒฉ์ž ์„ธ๋ถ„ํ™” ๊ธฐ๋ฒ• ๋ฐ ๋ณ‘๋ ฌ ์ฒ˜๋ฆฌ ๊ธฐ๋ฒ•์„ ์ ์šฉํ•˜์˜€๋‹ค. ๊ฐœ๋ฐœ๋œ ์ฝ”๋“œ๋ฅผ ๋ฐ”ํƒ•์œผ๋กœ ๋‹ค์–‘ํ•œ ์—ด๋ถ€ํ•˜ ์‹œ์Šคํ…œ์˜ ๋ฐ˜์‘์„ฑ ์œ ๋™ ๋ฐ ๊ตฌ์กฐ์˜ ์ƒํ˜ธ์ž‘์šฉ์„ ํ•ด์„ํ•˜์˜€๋‹ค. ์ˆ˜์ง๋ฐœ์‚ฌ๋Œ€ ๋‚ด๋ถ€์—์„œ ๋ฐœ์‚ฌ๋˜๋Š” ๋กœ์ผ“ ํ™”์—ผ์— ์˜ํ•ด ๋ณ€ํ˜•๋˜๋Š” ๋ฐœ์‚ฌ๋Œ€ ํ•˜๋ถ€์˜ ํ›„๋ฐฉ ๋ฎ๊ฐœ ๊ฑฐ๋™์„ ํ•ด์„ ํ•˜์˜€๋‹ค. ํ•ด์„ ๊ฒฐ๊ณผ๋Š” ์‹คํ—˜๊ฐ’๊ณผ ๋น„๊ตํ•˜์—ฌ ๊ฒ€์ฆํ•˜์˜€๊ณ , ํ•ด์„ ๊ฒฐ๊ณผ๋ฅผ ํ†ตํ•ด ํ›„๋ฐฉ ๋ฎ๊ฐœ์˜ ๋ณ€ํ˜•์ด ์œ ๋™์— ๋ฏธ์น˜๋Š” ์˜ํ–ฅ์„ ํ™•์ธ ํ•˜์˜€๋‹ค. ๋˜ํ•œ 2์ฐจ์›์œผ๋กœ ๋‹จ์ˆœํ™” ํ•  ์ˆ˜ ์—†๋Š” 3์ฐจ์› ๋ฒ™์ปค ๋‚ด๋ถ€์—์„œ ๋ฐœ์ƒํ•˜๋Š” ๊ณ ์ฒด ํ™”์•ฝ์˜ ํญ๋ฐœ ํ˜„์ƒ๊ณผ ๋ฒฝ๋ฉด์œผ๋กœ ์ „๋‹ฌ๋˜๋Š” ์••๋ ฅ์„ ํ•ด์„ํ•˜์˜€๋‹ค. ํ•ด์„๊ฒฐ๊ณผ๋Š” ์‹คํ—˜๊ฐ’๊ณผ ๋น„๊ตํ•˜์—ฌ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ๊ธˆ์†๊ด€ ๋‚ด๋ถ€์—์„œ์˜ ํญ๋ฐœ์— ์˜ํ•œ ๊ด€ ๋ณ€ํ˜• ํ•ด์„์—์„œ๋Š” ๊ด€์˜ ์˜จ๋„์— ๋”ฐ๋ฅธ ํ•ญ๋ณต์‘๋ ฅ์„ ๊ณ ๋ คํ•˜์—ฌ ํ•ด์„ํ•˜์˜€๋‹ค. ๊ณ ์˜จ์˜ ํ™˜๊ฒฝ์— ๋…ธ์ถœ๋˜๋Š” Pulse Detonation Engine(PDE)์˜ ๊ฒฝ์šฐ์—๋Š” ์˜จ๋„๊ฐ€ ๊ณ ๋ ค๋œ ๋ฌผ์„ฑ์น˜๋ฅผ ์‚ฌ์šฉํ•˜์—ฌ์•ผ ์ •ํ™•ํ•œ ๊ฒฐ๊ณผ๋ฅผ ์–ป์„ ์ˆ˜ ์žˆ๊ณ  ์ด๋ก ์ ์ธ ํŒŒ๊ดด ๋ชจ๋ธ๊ณผ ๋น„๊ตํ•˜์—ฌ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ์œ ์ฒด-๊ณ ์ฒด ์—ฐ๋™ ํ•ด์„์— ์žˆ์–ด์„œ ์‹ค์ œ ํ˜„์ƒ์— ๋ณด๋‹ค ๊ทผ์ ‘ํ•˜๊ธฐ ์œ„ํ•˜์—ฌ ๋–จ๋ฆฌ๋Š” ๊ด€ ๋‚ด๋ถ€์—์„œ์˜ ๋ฐํ† ๋„ค์ด์…˜ ํ˜„์ƒ์„ ํ™•์ธํ•˜์˜€๋‹ค. PDE์˜ ๊ฒฝ์šฐ, ์—ฐ์†์ ์ธ ๋ฐํ† ๋„ค์ด์…˜์ด ๊ด€ ๋‚ด๋ถ€๋ฅผ ์ง€๋‚˜๊ธฐ ๋•Œ๋ฌธ์— ๊ด€์˜ ํŒŒ๊ดด๊ฐ€ ์ผ์–ด๋‚˜์ง€ ์•Š๋”๋ผ๋„ ๊ณ ์œ ์ง„๋™์ˆ˜๋กœ ๋–จ๋ฆฌ๊ณ  ์žˆ์„ ๊ฒƒ์„ ๊ฐ์•ˆํ•˜์—ฌ ๊ณ ์œ ์ง„๋™์ˆ˜๋กœ ๋–จ๋ฆฌ๋Š” ๊ด€ ๋‚ด๋ถ€์—์„œ์˜ ๋ฐํ† ๋„ค์ด์…˜์„ ํ•ด์„ํ•˜์˜€๋‹ค. ์ด๋ฅผ ํ†ตํ•ด ๋ฐํ† ๋„ค์ด์…˜์˜ ์ „ํŒŒ๊ฐ€ ๊ด€์˜ ๋ณ€ํ˜•์— ์˜ํ–ฅ์„ ๋ฐ›๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€๋‹ค.Contents Abstract i Contents iii List of Tables vii List of Figures viii Preface xiv Chapter 1. Introduction 1 Chapter 2. Numerical Method 5 2.1 Governing equations and constitutive relations 5 2.1.1 Two-dimensional Eulerian coordinate system 5 2.1.2 Three-dimensional Eulerian coordinate system 7 2.1.3 Lagrangian coordinate system 9 2.2 Interface tracking and treatment method 12 2.2.1 Level conversion method 13 2.2.3 Ghost fluid method 16 2.2.4 Fluid-solid interaction algorithm 19 2.3 Advanced numerical technics for 3D simulation 20 Chapter 3. Validation 25 3.1 Gaseous energetic materials 25 3.1.1 Kerosene-air mixture 25 3.2 Solid energetic materials 29 3.2.1 Anisotropic PETN 29 3.3 Structure deformation 46 3.3.1 Taylor impact problem 46 3.4 Fluid-structure interaction method 49 Chapter 4. Vertical Launching System 52 4.1 Background and motivation 52 4.2 Results and discussion 54 4.2.1 Incoming rocket plume modeling 54 4.2.2 Case I. Opening of the Rear Cover 57 4.2.3 Case II. Closure of the Opened Rear Cover after Launch 65 4.3 Conclusion 67 Chapter 5. Detonation in Concrete Building 69 5.1 Background and motivation 69 5.2 Results and discussion 71 Chapter 6. Detonation in Tube 78 6.1 Background and motivation 78 6.2 Validation of detonation-loaded tube 80 6.3 Detonation-loaded tube 81 6.4 Detonation in the elastic vibrating steel tube 93 Chapter 7. Conclusion 96 References 98 Abstract in Korean 107Docto
    corecore