1,901 research outputs found

    Optimal experimental designs for the exploration of reaction kinetic phase diagrams

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    Meta-heuristic algorithms in car engine design: a literature survey

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    Meta-heuristic algorithms are often inspired by natural phenomena, including the evolution of species in Darwinian natural selection theory, ant behaviors in biology, flock behaviors of some birds, and annealing in metallurgy. Due to their great potential in solving difficult optimization problems, meta-heuristic algorithms have found their way into automobile engine design. There are different optimization problems arising in different areas of car engine management including calibration, control system, fault diagnosis, and modeling. In this paper we review the state-of-the-art applications of different meta-heuristic algorithms in engine management systems. The review covers a wide range of research, including the application of meta-heuristic algorithms in engine calibration, optimizing engine control systems, engine fault diagnosis, and optimizing different parts of engines and modeling. The meta-heuristic algorithms reviewed in this paper include evolutionary algorithms, evolution strategy, evolutionary programming, genetic programming, differential evolution, estimation of distribution algorithm, ant colony optimization, particle swarm optimization, memetic algorithms, and artificial immune system

    ํŒŒ๋ผ๋ฏธํ„ฐ ์ถ”์ •์„ ํ†ตํ•œ ๋ถˆ๊ท ์ผ๊ณ„ ์ด‰๋งค ๋ฐ˜์‘์˜ ๋งˆ์ดํฌ๋กœํ‚ค๋„คํ‹ฑ ๋ชจ๋ธ๋ง

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ํ™”ํ•™์ƒ๋ฌผ๊ณตํ•™๋ถ€, 2021.8. ์ด์›๋ณด.์ตœ๊ทผ์— ๊ณ„์†ํ•ด์„œ ํ™˜๊ฒฝ ์˜ค์—ผ ๋ฌธ์ œ๊ฐ€ ๋Œ€๋‘๋จ์— ๋”ฐ๋ผ ์ด์‚ฐํ™”ํƒ„์†Œ๋ฅผ ์ค„์ด๋Š” ๊ฒƒ์— ๋Œ€ํ•œ ๊ด€์‹ฌ์ด ์ปค์ง€๊ณ  ์žˆ๋‹ค. ์ด์— ๋”ฐ๋ผ ๋‹ค์–‘ํ•œ ๋ถ„์•ผ์˜ ๋งŽ์€ ์—ฐ๊ตฌ์ž๋“ค๊ณผ ์‚ฐ์—…์—์„œ๋„ ์ด์‚ฐํ™”ํƒ„์†Œ์˜ ๋ฐฐ์ถœ์„ ์ค„์ด๊ณ ์ž ๋…ธ๋ ฅํ•˜๊ณ  ์žˆ๋‹ค. ํŠนํžˆ ํ™”ํ•™๊ณตํ•™์ž๋“ค์€ ์˜จ์‹ค ๊ฐ€์Šค๋ฅผ ์‚ฌ์šฉํ•˜์—ฌ ์œ ์šฉํ•œ ์ผ€๋ฏธ์ปฌ์„ ์ƒ์‚ฐํ•  ์ˆ˜ ์žˆ๋Š” ํƒ„์†Œ ํ™œ์šฉ ๋ฐ˜์‘ ๊ณต์ •๋“ค์„ ๊ฐœ๋ฐœํ•ด์™”๋‹ค. ์ด๋Ÿฌํ•œ ๋ฐ˜์‘๋“ค์— ๋Œ€ํ•ด ์ด๋ฏธ ์ƒ์šฉ ๊ณต์ •๋“ค์ด ๊ฐœ๋ฐœ๋˜์–ด ์žˆ์ง€๋งŒ ์ด ๋ฐ˜์‘๋“ค์˜ ๋ฐ˜์‘ ๋ฉ”์ปค๋‹ˆ์ฆ˜์— ๋Œ€ํ•ด์„œ๋Š” ์—ฌ์ „ํžˆ ๋…ผ์Ÿ์ด ์ง„ํ–‰ ์ค‘์ด๋‹ค. ์ปดํ“จํ„ฐ ๊ณ„์‚ฐ ์„ฑ๋Šฅ์˜ ๋ฐœ์ „๊ณผ ๋”๋ถˆ์–ด ๋ฐ˜์‘ ๋ฉ”์ปค๋‹ˆ์ฆ˜ ํƒ์ƒ‰์— ๋Œ€ํ•œ ์—ฐ๊ตฌ๋Š” ์ƒˆ๋กœ์šด ๊ตญ๋ฉด์„ ๋งž์•„ ๋”์šฑ ํ™œ๋ฐœํ•ด์ง€๊ณ  ์žˆ๋‹ค. ์ƒ๋‹นํ•œ ๊ณ„์‚ฐ๋Ÿ‰์„ ์š”๊ตฌํ•˜๋Š” ๊ณ„์‚ฐ ํ™”ํ•™์€ ๋ฐ˜์‘ ๋ฉ”์ปค๋‹ˆ์ฆ˜ ๋ถ„์„์— ์—„์ฒญ๋‚œ ๋„์›€์ด ๋˜๊ณ  ์žˆ๋‹ค. ๋”์šฑ์ด ํ‚ค๋„คํ‹ฑ ๊ด€์ ์—์„œ ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ๋ถ„์„ํ•  ์ˆ˜ ์žˆ๋Š” ๋งˆ์ดํฌ๋กœํ‚ค๋„คํ‹ฑ ์Šคํ„ฐ๋””๋Š” ๊ณ„์‚ฐ ํ™”ํ•™์˜ ๋ฐœ์ „๊ณผ ๋”๋ถˆ์–ด ์‹œ๋„ˆ์ง€ ํšจ๊ณผ๋ฅผ ๋‚ผ ์ˆ˜ ์žˆ๋‹ค. ํ™”ํ•™ ๊ณตํ•™์—์„œ ์ „ํ†ต์ ์ธ ํ‚ค๋„คํ‹ฑ ๋ชจ๋ธ์€ ์ฃผ๋กœ ๊ณต์ • ๊ฐœ๋ฐœ์— ์‚ฌ์šฉ๋˜๋Š” ๋ฐ˜๋ฉด, ๋งˆ์ดํฌ๋กœํ‚ค๋„คํ‹ฑ ๋ชจ๋ธ์€ ์ด๋Ÿฌํ•œ ์žฅ์ ์— ๋”ํ•˜์—ฌ ๊ทผ๋ณธ์ ์ธ ๋ถ„์„์ด ๊ฐ€๋Šฅํ•˜๋‹ค. ์ด๋Ÿฌํ•œ ์ด์œ ๋กœ ๋„๋ฆฌ ์•Œ๋ ค์ง„ ๋ฐ˜์‘๋“ค์— ๋Œ€ํ•ด์„œ๋„ ๋งˆ์ดํฌ๋กœํ‚ค๋„คํ‹ฑ์„ ํ†ตํ•œ ๋ฉ”์ปค๋‹ˆ์ฆ˜ ๋ถ„์„์€ ํ™œ๋ฐœํ•˜๊ฒŒ ์ด๋ฃจ์–ด์ง€๊ณ  ์žˆ๋‹ค. ๋ณธ ํ•™์œ„ ๋…ผ๋ฌธ์—์„œ๋Š” ๊ธฐ์กด์˜ ๋ช‡ ๊ฐ€์ง€ ๊ฒฐ์ ๋“ค์„ ๊ฐœ์„ ํ•  ์ˆ˜ ์žˆ๋Š” ์‹ค์šฉ์ ์ธ ๋งˆ์ดํฌ๋กœํ‚ค๋„คํ‹ฑ ๋ชจ๋ธ๋ง ์ „๋žต์„ ์ œ์•ˆํ•˜์˜€๋‹ค. ๋ฉ”ํƒ„์˜ฌ ๋ฐ ๋””๋ฉ”ํ‹ธ์—ํ…Œ๋ฅด(DME) ํ•ฉ์„ฑ ๊ด€๋ จ ๋ฐ˜์‘๋“ค์— ๋Œ€ํ•ด์„œ ๋ฐ€๋„๋ฒ”ํ•จ์ˆ˜ ์ด๋ก (DFT) ๋ฐ ์ด ๊ฒฐ๊ณผ๋ฅผ ์ด์šฉํ•œ ๋งˆ์ดํฌ๋กœํ‚ค๋„คํ‹ฑ ๋ชจ๋ธ๋ง์„ ์ˆ˜ํ–‰ํ•˜๊ณ , ์ด๋ฅผ ํ†ตํ•œ ๋ฐ˜์‘ ๋ฉ”์ปค๋‹ˆ์ฆ˜ ๋ถ„์„ ๋ฐ ์—ฌ๋Ÿฌ ์ผ€์ด์Šค ์Šคํ„ฐ๋””๋ฅผ ์ง„ํ–‰ํ•˜์˜€๋‹ค. ํŒŒ๋ผ๋ฏธํ„ฐ ์ถ”์ • ๊ธฐ๋ฒ•์„ ์ด์šฉํ•˜์—ฌ ์˜ˆ์ธก๊ฐ’๊ณผ ์‹คํ—˜๊ฐ’์˜ ์ฐจ์ด๋ฅผ ์ตœ์†Œํ™” ํ•˜๋Š” ๋ฐฉํ–ฅ์œผ๋กœ Pre-exponential ์ธ์ž๋ฅผ ์‹คํ—˜ ๋ฐ์ดํ„ฐ์— ํ”ผํŒ…ํ•˜์˜€๋‹ค. ์ด๋Ÿฌํ•œ ๋งˆ์ดํฌ๋กœํ‚ค๋„คํ‹ฑ์Šค์—์˜ ์‹ค์šฉ์ ์ธ ๋ชจ๋ธ๋ง ์ ‘๊ทผ๋ฒ•์€ ๋ชจ๋ธ์˜ ๊ณ„์‚ฐํšจ์œจ๊ณผ ์‹ ๋ขฐ์„ฑ์„ ๊ฐœ์„ ํ•  ์ˆ˜ ์žˆ์—ˆ๋‹ค. ๋…ผ๋ฌธ์˜ ์ฒซ ๋ฒˆ์งธ ๋ถ€๋ถ„์œผ๋กœ Lumped ํ‚ค๋„คํ‹ฑ ๋ชจ๋ธ๊ณผ ๋งˆ์ดํฌ๋กœํ‚ค๋„คํ‹ฑ ๋ชจ๋ธ์˜ ์ฐจ์ด๋ฅผ ๊ฐ•์กฐํ•˜๊ธฐ ์œ„ํ•ด, Cu/ZnO/Al2O3/ferrierite (CZA/FER) ํ•˜์ด๋ธŒ๋ฆฌ๋“œ ์ด‰๋งค ํ•˜์—์„œ ํ•ฉ์„ฑ๊ฐ€์Šค๋กœ๋ถ€ํ„ฐ ๋””๋ฉ”ํ‹ธ์—ํ…Œ๋ฅด๋กœ์˜ ์ง์ ‘ ์ „ํ™˜ ๋ฐ˜์‘์— ๋Œ€ํ•ด Lumped ํ‚ค๋„คํ‹ฑ ๋ชจ๋ธ์„ ๊ฐœ๋ฐœํ•˜์˜€๋‹ค. ํ‚ค๋„คํ‹ฑ ํŒŒ๋ผ๋ฏธํ„ฐ๋Š” ํ•˜์ด๋ธŒ๋ฆฌ๋“œ ์ด‰๋งค์—์„œ์˜ ์‹คํ—˜ ๊ฐ’์— ํ”ผํŒ…๋˜๋„๋ก ์ถ”์ •ํ•˜์˜€๊ณ , ์ด๋Š” CZA ๋ฐ FER ์ด‰๋งค ๊ฐ๊ฐ์—์„œ ๋ณด๊ณ ๋œ ์„ ํ–‰ ์—ฐ๊ตฌ์—์„œ์˜ ๊ฐ’๊ณผ ๋น„๊ตํ•˜์˜€๋‹ค. ํ•˜์ด๋ธŒ๋ฆฌ๋“œ ์ด‰๋งค์—์„œ์˜ ๋†’์€ ํ™œ์„ฑํ™” ์—๋„ˆ์ง€๋Š” ๋ฉ”ํƒ„์˜ฌ ํ•ฉ์„ฑ ๋‹จ๊ณ„๊ฐ€ ๋ฉ”ํƒ„์˜ฌ ํƒˆ์ˆ˜ ๋‹จ๊ณ„๋ณด๋‹ค ์ „์ฒด์ ์ธ ๋ฐ˜์‘ ์†๋„๋ฅผ ์กฐ์ ˆํ•˜๋Š” ์ธ์ž๋ผ๋Š” ๊ฒƒ์„ ๋ณด์—ฌ์ฃผ์—ˆ๋‹ค. ๋˜ํ•œ ๊ฐœ๋ฐœ๋œ ํ‚ค๋„คํ‹ฑ ๋ชจ๋ธ์„ ํ†ตํ•ด 200 ~ 220 โ„ƒ์˜ ์˜จ๋„์—์„œ ์šด์ „ํ•˜๋Š” ๊ฒƒ์ด ํšจ์œจ์ ์ž„์„ ์•Œ ์ˆ˜ ์žˆ์—ˆ์œผ๋ฉฐ, ์ตœ์ ์˜ ์šด์ „ ์••๋ ฅ ๋ฐ ๊ณต๊ฐ„ ์†๋„๋ฅผ ์ œ์‹œํ•˜์˜€๋‹ค. ๋‘ ๋ฒˆ์งธ ๋ถ€๋ถ„์—์„œ๋Š” ๊ตฌ๋ฆฌ ๊ธฐ๋ฐ˜ ์ด‰๋งค ํ•˜์—์„œ ํ•ฉ์„ฑ๊ฐ€์Šค๋กœ๋ถ€ํ„ฐ ๋ฉ”ํƒ„์˜ฌ์„ ํ•ฉ์„ฑํ•˜๋Š” ๋ฐ˜์‘์— ๋Œ€ํ•ด์„œ ๋งˆ์ดํฌ๋กœํ‚ค๋„คํ‹ฑ ๋ชจ๋ธ๋ง์„ ํ•˜๊ธฐ ์œ„ํ•œ ์‹ค์šฉ์ ์ธ ๋ฐฉ๋ฒ•์— ๋Œ€ํ•ด ๋ฌ˜์‚ฌํ•˜์˜€๋‹ค. ์ผ์‚ฐํ™”ํƒ„์†Œ ๋ฐ ์ด์‚ฐํ™”ํƒ„์†Œ์˜ ์ˆ˜์†Œํ™” ๋ฐ˜์‘, Water-gas shift ๋ฐ˜์‘์— ๋Œ€ํ•ด 28๊ฐœ์˜ ๋‹จ์ผ๋‹จ๊ณ„๋ฐ˜์‘์„ ๊ณ ๋ คํ•˜์˜€๋‹ค. DFT์™€ ๋ฐ˜๊ฒฝํ—˜์ ์ธ ๋ฐฉ๋ฒ•๋ก ์ธ Unity bond index-quadratic exponential (UBI-QEP) ๊ธฐ๋ฒ•์„ ์กฐํ•ฉํ•˜์—ฌ ํก์ฐฉ์—ด ๋ฐ ํ™œ์„ฑํ™” ์—๋„ˆ์ง€๋ฅผ ๋„์ถœํ•˜์˜€๋‹ค. DFT ๊ณ„์‚ฐ์„ ํ†ตํ•ด ํฌ๋ฆ„์‚ฐ์—ผ(HCOO**)์ด ์ด์ขŒ๋ฐฐ์œ„์ž(Bidentate) ํ˜•ํƒœ๋กœ ํก์ฐฉ๋˜๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€์œผ๋ฉฐ, UBI-QEP ๊ณ„์‚ฐ์„ ์œ„ํ•œ ๊ธฐ์ƒ๊ณผ ํก์ฐฉ๋œ ์ค‘๊ฐ„ ์ƒ์„ฑ๋ฌผ๋“ค์˜ ํก์ฐฉ์—๋„ˆ์ง€ ๋ฐ ์—”ํƒˆํ”ผ๋ฅผ ์ œ๊ณตํ•˜์˜€๋‹ค. Pre-exponential ์ธ์ž์˜ ๊ฒฝ์šฐ์—๋Š” ์ „์ด์ƒํƒœ์ด๋ก ์˜ Order-of-magnitude์— ๊ธฐ๋ฐ˜ํ•˜์—ฌ ์ดˆ๊ธฐ ๊ฐ’์„ ์„ค์ •ํ•˜๊ณ , ์‹คํ—˜ ๋ฐ์ดํ„ฐ์— ํ”ผํŒ…ํ•˜์˜€๋‹ค. ๋•๋ถ„์— ์ด๋ฅผ ์œ„ํ•œ ์ง„๋™ ์ฃผํŒŒ์ˆ˜ ๋ฐ ๋ถ„๋ฐฐ ํ•จ์ˆ˜๋ฅผ ๊ณ„์‚ฐํ•˜์ง€ ์•Š์•„ ๊ณ„์‚ฐ ๋กœ๋“œ๋ฅผ ์ค„์ผ ์ˆ˜ ์žˆ์—ˆ๋‹ค. ๋ฐ˜์‘๊ธฐ ๋ชจ๋ธ์—์„œ๋Š” ๋งˆ์ดํฌ๋กœํ‚ค๋„คํ‹ฑ ๋ชจ๋ธ์˜ ๊ฒฝ์ง์„ฑ์„ ์™„ํ™”ํ•˜๊ธฐ ์œ„ํ•ด ๋ถ€๋ถ„ํ‰ํ˜•๋น„๋ฅผ ๊ณ„์‚ฐํ•˜์˜€๋‹ค. ์ƒ๋Œ€์ ์œผ๋กœ ๋น ๋ฅธ ๋‹จ์ผ๋‹จ๊ณ„๋ฐ˜์‘์„ ๊ธฐ๋ฐ˜์œผ๋กœ ์šฐ์„ธํ•œ ๋ฐ˜์‘ ๊ฒฝ๋กœ๋ฅผ ์ œ์•ˆํ•˜์˜€์œผ๋ฉฐ, Degree of rate control ๊ณ„์‚ฐ์„ ํ†ตํ•ด H3CO*์™€ H*์˜ ํ‘œ๋ฉด ๋ฐ˜์‘์ด ์†๋„ ๊ฒฐ์ • ๋‹จ๊ณ„์ž„์„ ์ œ์•ˆํ•˜์˜€๋‹ค. ๋˜ํ•œ ์šด์ „ ์˜จ๋„, ์••๋ ฅ ๋ฐ Feed์˜ H2 ๋ถ„์œจ์ด ๋ฉ”ํƒ„์˜ฌ ํ•ฉ์„ฑ ์†๋„์— ๋ฏธ์น˜๋Š” ์˜ํ–ฅ์„ ์•Œ์•„๋ณด๊ธฐ ์œ„ํ•ด ๊ฐœ๋ฐœ๋œ ๋ชจ๋ธ์„ ์‚ฌ์šฉํ•˜์˜€๋‹ค. ์„ธ ๋ฒˆ์งธ ๋ถ€๋ถ„์—์„œ๋Š” ๊ณ„์‚ฐ ํ™”ํ•™ ๋ฐ ๋งˆ์ดํฌ๋กœํ‚ค๋„คํ‹ฑ ๋ชจ๋ธ๋ง์„ ํ†ตํ•ด, H-zeolite ์ด‰๋งค ํ•˜์—์„œ ๋ฉ”ํƒ„์˜ฌ ํƒˆ์ˆ˜ ๋ฐ˜์‘์— ์˜ํ•œ ๋””๋ฉ”ํ‹ธ์—ํ…Œ๋ฅด ํ•ฉ์„ฑ์— ๋Œ€ํ•ด์„œ ๋ฐ˜์‘ ๊ฒฝ๋กœ๋ฅผ ๋ถ„์„ํ•˜์˜€๋‹ค. ๋ฐ˜์‘ ๋ฉ”์ปค๋‹ˆ์ฆ˜์œผ๋กœ๋Š” Associative ๋ฐ Dissociative ๊ฒฝ๋กœ์— ๋Œ€ํ•ด์„œ 9๊ฐœ์˜ ๋‹จ์ผ๋‹จ๊ณ„๋ฐ˜์‘์„ ํฌํ•จํ•˜์˜€๋‹ค. ์ด๋Ÿฌํ•œ ๋ฐ˜์‘ ์‹œ์Šคํ…œ์—์„œ๋Š” ๋ถ„์‚ฐ๋ ฅ์˜ ์˜ํ–ฅ์ด ์žˆ์œผ๋ฏ€๋กœ 2์ฐจ ๋ฌ„๋Ÿฌ-ํ”Œ๋ ˆ์…‹ ์„ญ๋™ ์ด๋ก (MP2)์— ๊ธฐ๋ฐ˜ํ•˜์—ฌ ๋ฐ˜์‘์ข…๋“ค์˜ ๊ตฌ์กฐ๋ฅผ ์ตœ์ ํ™”ํ•˜์˜€๋‹ค. ๋˜ํ•œ, ๋ฐ˜์‘์˜ ์ „์ด ์ƒํƒœ๋ฅผ ๋„์ถœํ•˜์˜€์œผ๋ฉฐ ์ด์™€ ์ตœ์  ๋ถ„์ž ๊ตฌ์กฐ์˜ ์—๋„ˆ์ง€ ๋ฐ ํ™œ์„ฑํ™” ์—๋„ˆ์ง€๋ฅผ ๊ณ„์‚ฐํ•˜์˜€๋‹ค. ์ด ๊ฒฐ๊ณผ์— ๊ธฐ๋ฐ˜ํ•˜์—ฌ ๋งˆ์ดํฌ๋กœํ‚ค๋„คํ‹ฑ ๋ชจ๋ธ์„ ๊ฐœ๋ฐœํ•˜์˜€๊ณ , Pre-exponential ์ธ์ž๋Š” ๋งˆ์ฐฌ๊ฐ€์ง€๋กœ ์‹คํ—˜ ๋ฐ์ดํ„ฐ์— ํ”ผํŒ…ํ•˜์˜€๋‹ค. ์ด๋Ÿฌํ•œ ๋ฐฉ๋ฒ•๋ก ์€ ๊ฐœ๋ฐœ๋œ ๋งˆ์ดํฌ๋กœํ‚ค๋„คํ‹ฑ ๋ชจ๋ธ์˜ ์‹ ๋ขฐ์„ฑ์„ ๊ฐ•ํ™”ํ•˜์˜€๋‹ค. ๋‹จ์ผ๋‹จ๊ณ„๋ฐ˜์‘๋“ค์˜ ์ƒ๋Œ€์ ์ธ ๋ฐ˜์‘ ์†๋„๋ฅผ ๋น„๊ตํ•˜์—ฌ Dissociative ๊ฒฝ๋กœ๊ฐ€ ์šฐ์„ธํ•˜๊ฒŒ ์ž‘์šฉํ•จ์„ ์•Œ ์ˆ˜ ์žˆ์—ˆ์œผ๋ฉฐ, ์ด ๊ฒฝ๋กœ์˜ DME ์ƒ์„ฑ ๋ฐ˜์‘(CH3OH-CH3-Z โ†’ CH3OCH3-H-Z)์„ ์†๋„ ๊ฒฐ์ • ๋‹จ๊ณ„๋กœ ์ œ์•ˆํ•˜์˜€๋‹ค. ๋งˆ์ฐฌ๊ฐ€์ง€๋กœ ์ด ๋ชจ๋ธ์„ ํ†ตํ•ด ์˜จ๋„๊ฐ€ ์ด‰๋งค ํ‘œ๋ฉด์˜ ๋†๋„ ๋ถ„ํฌ์— ๋ฏธ์น˜๋Š” ์˜ํ–ฅ์„ ๋ถ„์„ํ•˜์˜€๋‹ค. ๋งˆ์ง€๋ง‰์œผ๋กœ, Water-gas shift ๋ฐ˜์‘์— ๋Œ€ํ•œ ๋งˆ์ดํฌ๋กœํ‚ค๋„คํ‹ฑ ๋ชจ๋ธ์— ๋Œ€ํ•˜์—ฌ ๊ธฐ๊ณ„ํ•™์Šต ๊ธฐ๋ฐ˜์˜ ๋Œ€์ฒด ๋ชจ๋ธ์„ ์ œ์‹œํ•˜์˜€๋‹ค. ๋งˆ์ดํฌ๋กœํ‚ค๋„คํ‹ฑ ๋Œ€์ฒด ๋ชจ๋ธ์€ ๋งˆ์ดํฌ๋กœํ‚ค๋„คํ‹ฑ์Šค์™€ ์ „์‚ฐ์œ ์ฒด์—ญํ•™์ด๋‚˜ ๊ณต์ • ์‹œ๋ฎฌ๋ ˆ์ด์…˜๊ณผ ๊ฐ™์€ ๋” ๋†’์€ ์ฐจ์›์˜ ๋ฐ˜์‘ ๊ณตํ•™ ๋ชจ๋“ˆ์„ ์ด์–ด์ฃผ๋Š” ๋‹ค๋ฆฌ ์—ญํ• ์„ ํ•  ์ˆ˜ ์žˆ๋‹ค. ExtraTrees ์•Œ๊ณ ๋ฆฌ์ฆ˜๊ณผ ์ธ๊ณต์‹ ๊ฒฝ๋ง์„ ์ด์šฉํ•˜์—ฌ ๊ฐœ๋ฐœ๋œ ๋งˆ์ดํฌ๋กœํ‚ค๋„คํ‹ฑ ๋ชจ๋ธ๋กœ๋ถ€ํ„ฐ ์–ป์€ ๋ฐ์ดํ„ฐ์…‹์„ ํšŒ๊ท€ํ•˜์˜€๋‹ค. ๋ณด๊ฐ„ ๊ธฐ๊ณ„ํ•™์Šต ๊ธฐ๋ฒ• ์ค‘์—์„œ ์ธ๊ณต์‹ ๊ฒฝ๋ง์€ ํšŒ๊ท€ ๋ถ„์„์—์„œ ๋†’์€ ์„ฑ๋Šฅ์„ ๋‚ผ ์ˆ˜ ์žˆ๋Š” ๊ฒƒ์œผ๋กœ ์ž˜ ์•Œ๋ ค์ ธ ์žˆ๊ณ , ExtraTrees ์•Œ๊ณ ๋ฆฌ์ฆ˜์€ ํŠน์„ฑ ์ค‘์š”๋„๋ฅผ ๊ณ„์‚ฐ ํ•  ์ˆ˜ ์žˆ๋‹ค. ์ธ๊ณต์‹ ๊ฒฝ๋ง ๊ธฐ๋ฐ˜์˜ ๋Œ€์ฒด ๋ชจ๋ธ์€ ํ‰๊ท  ์˜ค์ฐจ์œจ 0.01%๋กœ ์ข‹์€ ์„ฑ๋Šฅ์„ ๋ณด์—ฌ์ฃผ์—ˆ๋‹ค. ExtraTrees ์ผ๊ณ ๋ฆฌ์ฆ˜์€ ํŠน์„ฑ ์ค‘์š”๋„๋ฅผ ์ธก์ •ํ•  ์ˆ˜ ์žˆ์–ด, Water-gas shift ๋ฐ˜์‘์—์„œ ์ค‘์š”ํ•œ ๋‹จ์ผ๋‹จ๊ณ„๋ฐ˜์‘๊ณผ ์ค‘์š”ํ•œ ์ด‰๋งค ํ‘œ๋ฉด์˜ ์ค‘๊ฐ„์ƒ์„ฑ๋ฌผ์„ ์ฐพ์•„๋‚ผ ์ˆ˜ ์žˆ์—ˆ๋‹ค.In recent years, as environmental issues continue to emerge, interest in carbon utilization where carbon dioxide is the primary species to be reduced is growing. Accordingly, many researchers and industries in various fields have tried to reduce carbon emissions into the atmosphere. In particular, chemical engineers have developed carbon utilizing reaction processes which produce a variety of useful chemicals by consuming the greenhouse gases. Although the commercial processes related to these reactions have already been developed, controversy over their reaction mechanisms is still ongoing. Along with advances in computational performance, researches on reaction mechanism exploration are becoming more active in a new phase. Computational chemistry, which requires high computational costs, is a great help for reaction mechanism analysis. Moreover, microkinetic study is a study that can analyze mechanisms from a kinetic perspective, creating synergies along with improvements in computational chemistry. While conventional kinetic models in chemical engineering have been mainly used in terms of process design, microkinetic models, in addition to these advantages, allow fundamental analysis. For these reasons, mechanism analysis through microkinetics is actively underway even for common reactions. In this thesis, practical microkinetic modeling strategies that could improve several previous drawbacks were proposed. For reactions related to methanol and dimethyl ether (DME) synthesis, density functional theory (DFT) calculations and microkinetic modeling using the DFT results were conducted, and the reaction mechanism analysis and the several case studies were suggested. By using parameter estimation techniques, pre-exponential factors were fitted to experimental data minimizing the differences between the predicted and the experimental values. This practical modeling approach to the microkinetics improved computational efficiency and reliability of the model. In the first part, a lumped kinetic model for the direct synthesis of dimethyl ether from syngas over Cu/ZnO/Al2O3/ferrierite (CZA/FER) catalyst was presented to highlight the difference from a microkinetic model. Kinetic parameters were estimated by fitting experimental data for the hybrid catalyst, and these were compared with the reported values of conventional catalysts, which were the respective CZA and FER catalysts. High activation energies for the hybrid catalyst showed that the methanol synthesis step may have more control over the rate than the methanol dehydration step. Using the developed kinetic model, a temperature between 200 and 220 ยฐC was determined for thermal energy efficiency, and a further analysis provided the optimal range of the total pressure and space velocity. A practical strategy to develop a microkinetic model for methanol synthesis from syngas over a Cu-based catalyst is described in the second part. The comprehensive model consists of forward and backward reactions of 28 possible elementary-step reactions for CO and CO2 hydrogenation and the waterโ€“gas shift reaction. A combination of ab-initio DFT and semi-empirical unity bond index-quadratic exponential (UBI-QEP) methods was used to determine the heat of adsorption and activation energies. DFT calculations confirmed that formate (HCOO**) adsorbs in a bidentate fashion and provided the enthalpies and adsorption energies of gas and surface intermediates for subsequent UBI-QEP calculations. The pre-exponential factors were estimated from the order-of-magnitude of the transition state theory as the initial values and by fitting the experimental data, thus reducing the computational load by not calculating the vibrational frequencies and partition functions for translational, rotational, and vibrational motions. For the reactor model, partial equilibrium ratios were used to reduce the stiffness of the microkinetic model. The most plausible reaction pathways were suggested by considering relatively fast step-reactions, while the surface reaction of H3CO* and H* was found to be the rate-determining step by the degree of rate control. The developed model was also used to evaluate the effects of the temperature, pressure, and H2 fraction in the feed on the methanol synthesis rate to elucidate the suitable operating conditions. In the third part, the reaction pathways of DME synthesis by methanol dehydration over a H-zeolite catalyst were analyzed through both computational chemistry and microkinetic modeling methods. The reaction mechanisms consisted of nine elementary-step reactions for both associative and dissociative pathways. Based on the second-order Mรธllerโ€“Plesset perturbation theory (MP2), to determine the effects of dispersion forces that were important in this reaction system, the structures of all related reaction species were optimized, and the transition states of the associative and dissociative pathways were elucidated. Also, the energies and activation barriers of the optimized structures and transition states were calculated. Then, a microkinetic model was developed using the energies and activation barriers obtained from the MP2 calculations. Meanwhile, the pre-exponential factors of the kinetic parameters were not calculated theoretically but estimated by fitting the experimental data, which enhanced the reliability of the microkinetic model. By comparing the relative elementary-step reaction rates calculated using the developed model, the dissociative pathway was suggested as a dominant pathway of DME synthesis, while the DME formation reaction of the dissociative pathway (CH3OH-CH3-Z โ†’ CH3OCH3-H-Z) was found to be the rate-determining step. The developed model was also used to evaluate the effects of temperature on the site fractions over the catalyst. Finally, machine learning-based surrogate models of the microkinetic model for the water-gas shift reaction were developed. The surrogate model can play a role in a bridge between the microkinetics and the higher-scale reaction engineering modules such as computational fluid dynamics or process simulations. The ExtraTrees algorithm and the artificial neural network (ANN) were used for regressing the datasets acquired from the developed microkinetic model. Among interpolative machine learning techniques, an ANN is well known for its high performance in regression, and the feature importance can be calculated with the ExtraTrees algorithm. As a result, the ANN showed the great performance with an average error of 0.01 %. ExtraTrees could measure the feature importance, so that the important elementary reactions and surface intermediates to the overall reaction of the water-gas shift reaction were figured out.Chapter 1 Introduction 16 1.1 Research Motivation 16 1.2 Outline of the Thesis 18 1.3 Associated Publications 18 Chapter 2 Background Theory 19 2.1 Microkinetics 19 2.2 Kinetic Parameter 22 2.2.1 Computational Chemistry 24 2.2.2 Transition State Theory 25 2.2.3 UBI-QEP 28 Chapter 3 Lumped kinetic modeling for direct synthesis of DME from syngas 30 3.1 Background 30 3.2 Methods 34 3.2.1 Experimentals 34 3.2.2 Kinetic Model 37 3.3 Application Results and Discussion 42 Chapter 4 Microkietic modeling of methanol synthesis from syngas 53 4.1 Background 53 4.2 Reaction Mechanism 59 4.3 Methods 63 4.3.1 Activation Energy 63 4.3.2 Microkinetic Model 67 4.4 Application Results and Discussion 74 4.4.1 DFT Calculations 74 4.4.2 Microkinetic Model 78 4.4.3 Rate-Determining Step 88 4.4.4 Effects of Operating Conditions 89 Chapter 5 Microkinetic modeling of DME synthesis from methanol over H-zeolite catalyst 92 5.1 Background 92 5.2 Reaction mechanism 97 5.3 Methods 102 5.3.1 Computational Chemistry 102 5.3.2 Microkinetic Model 106 5.4 Application results and discussion 109 5.4.1 MP2 Calculations 109 5.4.2 Microkinetic Model 126 Chapter 6 Machine Learning-based Surrogate Model of Microkinetics for the Water-Gas Shift Reaction 136 6.1 Background 136 6.2 Reaction Mechanism 138 6.3 Methods 140 6.3.1 Microkinetic Model 140 6.3.2 Surrogate Model 143 6.4 Application Results and Discussion 148 6.4.1 Microkinetic Model 148 6.4.2 Surrogate Model 151 Chapter 7 Concluding Remarks 157 7.1 Summary of Contributions 157 7.2 Future Work 160 Appendix 162 Supporting Information 162 Bibliography 165 Abstract in Korean (๊ตญ๋ฌธ์ดˆ๋ก) 177๋ฐ•

    A Surrogate Model Assisted Evolutionary Algorithm for Computationally Expensive Design Optimization Problems with Discrete Variables

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    Real-world computationally expensive design optimization problems with discrete variables pose challenges to surrogate-based optimization methods in terms of both efficiency and search ability. In this paper, a new method is introduced, called surrogate model-aware differential evolution with neighbourhood exploration, which has two phases. The first phase adopts a surrogate-based optimization method based on efficient surrogate model-aware search framework, the goal of which is to reach at least the neighbourhood of the global optimum. In the second phase, a neighbourhood exploration method for discrete variables is developed and collaborates with the first phase to further improve the obtained solutions. Empirical studies on various benchmark problems and a real-world network-on-chip design optimization problem show the combined advantages in terms of efficiency and search ability: when only a very limited number of exact evaluations are allowed, the proposed method is not slower than one of the most efficient methods for the targeted problem; when more evaluations are allowed, the proposed method can obtain results with comparable quality compared to standard differential evolution, but it requires only 1% to 30% of exact function evaluations

    A Surrogate Model Assisted Evolutionary Algorithm for Computationally Expensive Design Optimization Problems with Discrete Variables

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    Real-world computationally expensive design optimization problems with discrete variables pose challenges to surrogate-based optimization methods in terms of both efficiency and search ability. In this paper, a new method is introduced, called surrogate model-aware differential evolution with neighbourhood exploration, which has two phases. The first phase adopts a surrogate-based optimization method based on efficient surrogate model-aware search framework, the goal of which is to reach at least the neighbourhood of the global optimum. In the second phase, a neighbourhood exploration method for discrete variables is developed and collaborates with the first phase to further improve the obtained solutions. Empirical studies on various benchmark problems and a real-world network-on-chip design optimization problem show the combined advantages in terms of efficiency and search ability: when only a very limited number of exact evaluations are allowed, the proposed method is not slower than one of the most efficient methods for the targeted problem; when more evaluations are allowed, the proposed method can obtain results with comparable quality compared to standard differential evolution, but it requires only 1% to 30% of exact function evaluations

    ๋ณต์žกํ•œ ๋™ํŠน์„ฑ์„ ๊ฐ–๋Š” ๋‹ค์ƒ ๋ฐ˜์‘๊ธฐ์˜ ์„ค๊ณ„๋ฅผ ์œ„ํ•œ ๊ณ„์‚ฐ ํšจ์œจ์ ์ธ ๋ชจ์‚ฌ ๋ฐ ์ตœ์ ํ™” ์ „๋žต

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :๊ณต๊ณผ๋Œ€ํ•™ ํ™”ํ•™์ƒ๋ฌผ๊ณตํ•™๋ถ€,2020. 2. ์ด์ข…๋ฏผ.๋ณธ ๋ฐ•์‚ฌํ•™์œ„๋…ผ๋ฌธ์—์„œ๋Š” ๋ฉ€ํ‹ฐ ์Šค์ผ€์ผ ๋ชจ๋ธ๋ง, ์‹คํ—˜ ๊ฒฐ๊ณผ๋ฅผ ์ด์šฉํ•œ ๋ชจ๋ธ ๋ณด์ •๋ฒ•, ์ตœ์ ํ™” ์ˆœ์œผ๋กœ ์ง„ํ–‰๋˜๋Š” ์‚ฐ์—…์šฉ ํ™”ํ•™ ๋ฐ˜์‘๊ธฐ์˜ ์„ค๊ณ„ ์ „๋žต์„ ์ œ์‹œํ•œ๋‹ค. ๋ฐ˜์‘๊ธฐ๋Š” ํ™”ํ•™ ๊ณต์ •์—์„œ ์ œ์ผ ์ค‘์š”ํ•œ ๋‹จ์œ„์ด์ง€๋งŒ, ๊ทธ ์„ค๊ณ„์— ์žˆ์–ด์„œ๋Š” ์ตœ์‹  ์ˆ˜์น˜์  ๊ธฐ๋ฒ•๋“ค๋ณด๋‹ค๋Š” ์—ฌ์ „ํžˆ ๊ฐ„๋‹จํ•œ ๋ชจ๋ธ์ด๋‚˜ ์‹คํ—˜ ๋ฐ ๊ฒฝํ—˜ ๊ทœ์น™์— ์˜์กดํ•˜๊ณ  ์žˆ๋Š” ํ˜„์‹ค์ด๋‹ค. ์‚ฐ์—… ๊ทœ๋ชจ์˜ ๋ฐ˜์‘๊ธฐ๋Š” ๋ฌผ๋ฆฌ, ํ™”ํ•™์ ์œผ๋กœ ๋ชน์‹œ ๋ณต์žกํ•˜๊ณ , ๊ด€๋ จ ๋ณ€์ˆ˜ ๊ฐ„์˜ ์Šค์ผ€์ผ์ด ํฌ๊ฒŒ ์ฐจ์ด๋‚˜๋Š” ๊ฒฝ์šฐ๊ฐ€ ๋งŽ์•„ ์ˆ˜ํ•™์  ๋ชจ๋ธ๋ง ๋ฐ ์ˆ˜์น˜์  ํ•ด๋ฒ•์„ ๊ตฌํ•˜๊ธฐ๊ฐ€ ์–ด๋ ต๋‹ค. ๋ชจ๋ธ์„ ๋งŒ๋“ค๋”๋ผ๋„ ๋ถ€์ •ํ™•ํ•˜๊ฑฐ๋‚˜ ์‹œ๋ฎฌ๋ ˆ์ด์…˜ ์‹œ๊ฐ„์ด ๋„ˆ๋ฌด ๊ธด ๋ฌธ์ œ๊ฐ€ ์žˆ์–ด ์ตœ์ ํ™” ์•Œ๊ณ ๋ฆฌ์ฆ˜์— ์ ์šฉํ•˜๊ธฐ๊ฐ€ ํž˜๋“ค๋‹ค. ๋ฐ˜์‘๊ธฐ ๋‚ด ํ˜„์ƒ์˜ ๋ณต์žก์„ฑ๊ณผ ์Šค์ผ€์ผ ์ฐจ์ด ๋ฌธ์ œ๋Š” ๋ฉ€ํ‹ฐ ์Šค์ผ€์ผ ๋ชจ๋ธ๋ง์„ ํ†ตํ•ด ์ ‘๊ทผํ•  ์ˆ˜ ์žˆ๋‹ค. ์ „์‚ฐ์œ ์ฒด์—ญํ•™ ๊ธฐ๋ฐ˜ ๊ตฌํš ๋ชจ๋ธ(CFD-based compartmental model)์„ ์ด์šฉํ•˜๋ฉด, ๋ถˆ๊ท ์ผํ•œ ํ˜ผํ•ฉ ํŒจํ„ด์„ ๋ณด์ด๋Š” ๋Œ€ํ˜• ๋ฐ˜์‘๊ธฐ์—์„œ๋„ ๊ธด ์‹œ๊ฐ„ ๋™์•ˆ์˜ ๋™์  ๋ชจ์‚ฌ๊ฐ€ ๊ฐ€๋Šฅํ•˜๋‹ค. ์ด ๋ชจ๋ธ์€ ํฐ ๋ฐ˜์‘๊ธฐ๋ฅผ ์™„๋ฒฝํ•˜๊ฒŒ ๊ท ์ผํ•œ ์ž‘์€ ๊ตฌํš๋“ค์˜ ๋„คํŠธ์›Œํฌ๋กœ ๊ฐ„์ฃผํ•˜๊ณ , ๊ฐ ๊ตฌํš์„ ๋ฐ˜์‘ ์†๋„์‹๋“ค๊ณผ CFD ๊ฒฐ๊ณผ๋กœ๋ถ€ํ„ฐ ๊ฐ€์ ธ์˜จ ์œ ๋™ ์ •๋ณด๊ฐ€ ํฌํ•จ๋œ ์งˆ๋Ÿ‰ ๋ฐ ์—๋„ˆ์ง€ ๊ท ํ˜• ๋ฐฉ์ •์‹์œผ๋กœ ํ‘œํ˜„ํ•œ๋‹ค. ๊ธฐ์ฒด, ์•ก์ฒด, ๊ณ ์ฒด 3์ƒ์ด ์ƒํ˜ธ์ž‘์šฉํ•˜๋ฉฐ ๋ณต์žกํ•œ ์œ ๋™์„ ๋ณด์ด๋Š” ์ˆ˜์„ฑ ๊ด‘๋ฌผ ํƒ„์‚ฐํ™” ๋ฐ˜์‘๊ธฐ๋ฅผ ์ด ๋ฐฉ๋ฒ•์„ ์‚ฌ์šฉํ•ด ๋ชจ๋ธ๋งํ•˜์˜€๋‹ค. ์ด ๋•Œ ๋ชจ๋ธ์€ ๋ฏธ๋ถ„ ๋Œ€์ˆ˜ ๋ฐฉ์ •์‹(DAE)์˜ ํ˜•ํƒœ๋ฅผ ๋ ๋ฉฐ, ๋ฉ”์ปค๋‹ˆ์ฆ˜ ์ƒ ๋ชจ๋“  ๋ฐ˜์‘๋“ค(๊ธฐ-์•ก ๊ฐ„ ๋ฌผ์งˆ ์ „๋‹ฌ ๋ฐ˜์‘, ๊ณ ์ฒด ์šฉํ•ด ๋ฐ˜์‘, ์ด์˜จ ๊ฐ„ ๋ฐ˜์‘, ์•™๊ธˆ ์นจ์ „ ๋ฐ˜์‘)๊ณผ ์œ ์ฒด ์—ญํ•™, ๋ฐ˜์‘์—ด, ์—ด์—ญํ•™์  ๋ณ€ํ™” ๋ฐ ์šด์ „ ์ƒ์˜ ์ด๋ฒคํŠธ ๋ฐœ์ƒ์„ ๋ชจ๋‘ ๊ณ ๋ คํ•  ์ˆ˜ ์žˆ๋‹ค. ๋ชจ๋ธ์„ ์ด์šฉํ•ด ์ด์‚ฐํ™”ํƒ„์†Œ ์ œ๊ฑฐ ํšจ์œจ, pH ๋ฐ ์˜จ๋„ ๋ณ€ํ™”๋ฅผ ์˜ˆ์ธกํ•˜์—ฌ ์‹ค์ œ ์šด์ „ ๋ฐ์ดํ„ฐ์™€ ๋น„๊ตํ•œ ๊ฒฐ๊ณผ, ํŒŒ๋ผ๋ฏธํ„ฐ๋ฅผ ํ†ตํ•œ ๋ณด์ •์ด ์ „ํ˜€ ์—†์ด๋„ 7 % ์ด๋‚ด์˜ ์˜ค์ฐจ๋ฅผ ๋ณด์—ฌ์ฃผ์—ˆ๋‹ค. ๋ชจ๋ธ์˜ ๋ถ€์ •ํ™•์„ฑ ๋ฌธ์ œ๋Š” ๋ชจ๋ธ๋ง ํ›„ ์‹คํ—˜ ๊ฒฐ๊ณผ๋ฅผ ์ด์šฉํ•œ ๋ชจ๋ธ ๋ณด์ •์œผ๋กœ ๊ทน๋ณต ํ•  ์ˆ˜ ์žˆ๋‹ค. ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ๊ด‘๋ฌผ ํƒ„์‚ฐํ™” ๋ฐ˜์‘๊ธฐ ๋ชจ๋ธ์„ ๋ฒ ์ด์ง€์•ˆ ๋ณด์ •(Bayesian calibration)์„ ํ†ตํ•ด ๊ฐ•ํ™”ํ•˜๋Š” ๋ฐฉ๋ฒ•์„ ์ œ์‹œํ•œ๋‹ค. ๋จผ์ € ๋ชจ๋ธ ์ค‘ ๋ถˆํ™•์‹คํ•œ ๋ถ€๋ถ„์— 8๊ฐœ์˜ ํŒŒ๋ผ๋ฏธํ„ฐ๋ฅผ ๋„์ž…ํ•œ ํ›„, ๋ฒ ์ด์ง€์•ˆ ํŒŒ๋ผ๋ฏธํ„ฐ ์ถ”์ •๋ฒ•(Bayesian parameter estimation) ๋ฐ ์‹คํ—˜์‹ค ๊ทœ๋ชจ์—์„œ์˜ ์‹คํ—˜ ๊ฒฐ๊ณผ๋“ค์„ ์ด์šฉํ•˜์—ฌ ํŒŒ๋ผ๋ฏธํ„ฐ๋“ค์˜ ์‚ฌํ›„ ํ™•๋ฅ  ๋ถ„ํฌ๋ฅผ ์ถ”์ •ํ•˜์˜€๋‹ค. ์–ป์–ด์ง„ ํŒŒ๋ผ๋ฏธํ„ฐ์˜ ํ™•๋ฅ  ๋ถ„ํฌ๋“ค์€ ๋ชจ๋ธ ๋ฐ ์‹คํ—˜์˜ ๋ถˆ์™„์ „์„ฑ์œผ๋กœ ์ธํ•ด ๋‚˜ํƒ€๋‚˜๋Š” ํŒŒ๋ผ๋ฏธํ„ฐ์˜ ๋ถˆํ™•์‹ค์„ฑ ๋ฐ ๋‹ค์ค‘ ๋ด‰์šฐ๋ฆฌ ํŠน์„ฑ์„ ๋ฐ˜์˜ํ•˜๊ณ  ์žˆ๋‹ค. ์ด๋ฅผ ์ด์šฉํ•˜์—ฌ ์‹คํ—˜ ๊ฒฐ๊ณผ๋ฅผ ์ž˜ ๋”ฐ๋ผ๊ฐ€๋Š” ํ™•๋ฅ ๋ก ์  ๋ชจ๋ธ ์˜ˆ์ธก์น˜(stochastic model response)๋ฅผ ์–ป์„ ์ˆ˜ ์žˆ์—ˆ๋‹ค. 16๊ฐœ์˜ ์‹คํ—˜ ๋ฐ์ดํ„ฐ์…‹ ๋ฐ ํ…Œ์ŠคํŠธ์…‹์˜ ํ”ผํŒ… ์—๋Ÿฌ(fitting error)๋Š” ๊ฒฐ์ •๋ก ์ ์ธ ์ตœ์ ํ™” ์•Œ๊ณ ๋ฆฌ์ฆ˜(deterministic optimization)์„ ์‚ฌ์šฉํ•  ๋•Œ๋ณด๋‹ค ๋น„์Šทํ•˜๊ฑฐ๋‚˜ ๋‚ฎ์€ ๊ฒƒ์œผ๋กœ ์ธก์ •๋˜์—ˆ๋‹ค. ์ˆ˜ํ•™์  ์ตœ์ ํ™”์— ์“ฐ์ด๊ธฐ์— ๋„ˆ๋ฌด ๊ธด ์‹œ๋ฎฌ๋ ˆ์ด์…˜ ์‹œ๊ฐ„ ๋ฌธ์ œ๋Š” ๋ฒ ์ด์ง€์•ˆ ์ตœ์ ํ™” ์•Œ๊ณ ๋ฆฌ์ฆ˜์„ ์ ์šฉํ•˜์—ฌ ํ•ด๊ฒฐํ•  ์ˆ˜ ์žˆ๋‹ค. ํ™”ํ•™ ๋ฐ˜์‘๊ธฐ ์„ค๊ณ„ ์ตœ์ ํ™”๋ฅผ ์œ„ํ•ด ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ๋‹ค์ค‘ ๋ชฉ์  ๋ฒ ์ด์ง€์•ˆ ์ตœ์ ํ™”(Multi-objective Bayesian Optimization, MBO)๋ฅผ ์‚ฌ์šฉํ•ด ์‹œ๋ฎฌ๋ ˆ์ด์…˜ ํšŸ์ˆ˜๋ฅผ ์ตœ์†Œํ™” ํ•˜๋Š” CFD ๊ธฐ๋ฐ˜ ์ตœ์  ์„ค๊ณ„ ๋ฐฉ๋ฒ•์„ ์ œ์•ˆํ•˜์˜€๋‹ค. ์—ฌ์„ฏ ๊ฐ€์ง€ ์„ค๊ณ„ ๋ณ€์ˆ˜๋ฅผ ๊ฐ€์ง€๋Š” ๊ธฐ-์•ก ๊ต๋ฐ˜ ํƒฑํฌ ๋ฐ˜์‘๊ธฐ์—์„œ ์ „๋ ฅ ์†Œ๋น„๋ฅผ ์ตœ์†Œํ™”ํ•˜๊ณ  ๊ฐ€์Šค ๋ถ„์œจ(gas holdup)๋ฅผ ๊ทน๋Œ€ํ™”ํ•˜๊ธฐ ์œ„ํ•ด ์ด ๋ฐฉ๋ฒ•์„ ์ด์šฉํ•œ ๊ฒฐ๊ณผ, ๋‹จ 100 ํšŒ์˜ ์‹œ๋ฎฌ๋ ˆ์ด์…˜ ๋งŒ์œผ๋กœ ์ตœ์  ํŒŒ๋ ˆํ†  ์ปค๋ธŒ(Pareto curve)๋ฅผ ์–ป์„ ์ˆ˜ ์žˆ์—ˆ๋‹ค. ์ œ์•ˆ๋œ ์ตœ์  ์„ค๊ณ„์•ˆ๋“ค์€ ๋ฌธํ—Œ์— ๋ณด๊ณ ๋œ ๊ธฐ์กด ๋ฐ˜์‘๊ธฐ๋“ค๊ณผ ๋น„๊ตํ•ด ๋›ฐ์–ด๋‚œ ์„ฑ๋Šฅ์„ ๋ณด์—ฌ์ฃผ์—ˆ๋‹ค. . ๋ณธ ๋…ผ๋ฌธ์„ ํ†ตํ•ด ์ œ์•ˆ๋œ CFD ๊ธฐ๋ฐ˜ ๊ตฌํš ๋ชจ๋ธ๋ง๋ฒ•, ๋ฒ ์ด์ง€์•ˆ ๋ชจ๋ธ ๋ณด์ •๋ฒ• ๋ฐ ๋ฒ ์ด์ง€์•ˆ ์ตœ์ ํ™” ๋ฐฉ๋ฒ•์€ ๋ณต์žกํ•œ ๋ฌผ๋ฆฌ์  ๋ฐ ํ™”ํ•™์  ํŠน์ง•์„ ๊ฐ–๋Š” ์‚ฐ์—… ๊ทœ๋ชจ์˜ ํ™”ํ•™ ๋ฐ˜์‘๊ธฐ์— ์ ์šฉ๋  ์ˆ˜ ์žˆ์„ ๊ฒƒ์œผ๋กœ ๊ธฐ๋Œ€๋œ๋‹ค.This thesis presents a design strategy for industrial-scale chemical reactors which consists of multi-scale modeling, post-modeling calibration, and optimization. Although the reactor design problem is a primary step in the development of most chemical processes, it has been relied on simple models, experiments and rules of thumbs rather than taking advantage of recent numerical techniques. It is because industrial-size reactors show high complexity and scale differences both physically and chemically, which makes it difficult to be mathematically modeled. Even after the model is constructed, it suffers from inaccuracies and heavy simulation time to be applied in optimization algorithms. The complexity and scale difference problem in modeling can be solved by introducing multi-scale modeling approaches. Computational fluid dynamics (CFD)-based compartmental model makes it possible to simulate hours of dynamics in large size reactors which show inhomogeneous mixing patterns. It regards the big reactor as a network of small zones in which perfect mixing can be assumed and solves mass and energy balance equations with kinetics and flow information adopted from CFD hydrodynamics model at each zone. An aqueous mineral carbonation reactor with complex gasโ€“liquidโ€“solid interacting flow patterns was modeled using this method. The model considers the gas-liquid mass transfer, solid dissolution, ionic reactions, precipitations, hydrodynamics, heat generation and thermodynamic changes by the reaction and discrete operational events in the form of differential algebraic equations (DAEs). The total CO2 removal efficiency, pH, and temperature changes were predicted and compared to real operation data. The errors were within 7 % without any post-adjustment. The inaccuracy problem of model can be overcome by post-modeling approach, such as the calibration with experiments. The model for aqueous mineral carbonation reactor was intensified via Bayesian calibration. Eight parameters were intrduced in the uncertain parts of the rigorous reactor model. Then the calibration was performed by estimating the parameter posterior distribution using Bayesian parameter estimation framework and lab-scale experiments. The developed Bayesian parameter estimation framework involves surrogate models, Markov chain Monte Carlo (MCMC) with tempering, global optimization, and various analysis tools. The obtained parameter distributions reflected the uncertain or multimodal natures of the parameters due to the incompleteness of the model and the experiments. They were used to earn stochastic model responses which show good fits with the experimental results. The fitting errors of all the 16 datasets and the unseen test set were measured to be comparable or lower than when deterministic optimization methods are used. The heavy simulation time problem for mathematical optimization can be resolved by applying Bayesian optimizaion algorithm. CFD based optimal design tool for chemical reactors, in which multi-objective Bayesian optimization (MBO) is utilized to reduce the number of required CFD runs, is proposed. The developed optimizer was applied to minimize the power consumption and maximize the gas holdup in a gas-sparged stirred tank reactor, which has six design variables. The saturated Pareto front was obtained after only 100 iterations. The resulting Pareto front consists of many near-optimal designs with significantly enhanced performances compared to conventional reactors reported in the literature. It is anticipated that the suggested CFD-based compartmental modeling, post-modeling Bayesian calibration, and Bayesian optimization methods can be applied in general industrial-scale chemical reactors with complex physical and chemical features.1. Introduction 1 1.1. Industrial-scale chemical reactor design 1 1.2. Role of mathematical models in reactor design 2 1.3. Intensification of reactor models through calibration 5 1.3.1. Bayesian parameter estimation 6 1.4. Optimization of the reactor models 7 1.4.1. Bayesian optimization 9 1.5. Aqueous mineral carbonation process : case study subject 10 1.6. Outline of the thesis 12 2. Multi-scale modeling of industrial-scale aqueous mineral carbonation reactor for long-time dynamic simulation 14 2.1. Objective 14 2.2. Experimental setup 15 2.3. Mathematical models 19 2.3.1. Reactor model 19 2.3.2. CFD model 28 2.3.3. Numerical setting 30 2.4. Results and discussions 32 2.4.1. CFD-based compartmental model for industrial-scale reactor. 32 2.4.2. Design and simulation of higher-scale reactors 42 2.5. Conclusions 47 3. Model intensification of aqueous mineral carbonation kinetics via Bayesian calibration 50 3.1. Objective 50 3.2. Experimental methods 51 3.2.1. Solution and gas preparation 51 3.2.2. Laboratory-scale mineral carbonation process 53 3.3. Mathematical models 56 3.3.1. Kinetics of aqueous mineral carbonation process 56 3.3.2. Differential algebraic equation (DAE) model for the reactor 65 3.3.3. Discrete events for simulation procedure 71 3.3.4. Numerical setting 72 3.4. Bayesian parameter estimation 72 3.4.1. Problem formulation 73 3.4.2. Bayesian posterior inference 76 3.4.3. Sampling 81 3.5. Results and discussions 82 3.5.1. Stochastic output response 82 3.5.2. Quality of parameter estimtates 86 3.5.3. Assessment of parameter uncertainties 91 3.5.4. Kinetics study with the proposed model parameters 99 3.6. Conclusions 103 4. Multi-objective optimization of chemical reactor design using computational fluid dynamics 106 4.1. Objective 106 4.2. Problem Formulation 107 4.3. Optimization scheme 113 4.3.1. Multi-objective optimization algorithm 113 4.3.2. CFD-MBO optimizer 120 4.4. CFD modeling 125 4.4.1. Tank specifications 125 4.4.2. Governing equations 125 4.4.3. Simulation methods 127 4.5. Results and discussion 128 4.5.1. CFD model validation 128 4.5.2. Optimization results 130 4.5.3. Analysis of optimal designs 139 4.6. Conclusions 144 5. Concluding Remarks 146 Bibliography 149 Abstract in Korean (๊ตญ๋ฌธ์ดˆ๋ก) 163Docto
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