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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

    ๋””์ ค ์—”์ง„์˜ ์„ฑ๋Šฅ๊ณผ ๋ฐฐ๊ธฐ ์ตœ์ ํ™”๋ฅผ ์œ„ํ•œ ์—ฐ์†Œ ๋””์ž์ธ ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ๊ธฐ๊ณ„๊ณตํ•™๋ถ€, 2021.8. ์ด๊ด‘ํ˜ธ.์ตœ๊ทผ ๋‚ด์—ฐ๊ธฐ๊ด€ ์„ฑ๋Šฅํ–ฅ์ƒ์„ ์œ„ํ•œ ์—ฐ๊ตฌ๋Š” ์—ฐ๋น„, ๋ฐฐ์ถœ๋Ÿ‰, ์†Œ์Œ, ์ง„๋™ ๋“ฑ์˜ ์ธก๋ฉด์— ์ดˆ์ ์ด ๋งž์ถฐ์ง€๊ณ  ์žˆ๋‹ค. ์—ฐ๋น„๋Š” ์ง€๊ตฌ์˜จ๋‚œํ™”์— ์˜ํ–ฅ์„ ์ค€ ์ด์‚ฐํ™”ํƒ„์†Œ ๋ฐฐ์ถœ ๊ฐ์†Œ์™€ ๊ด€๋ จ์ด ์žˆ๋‹ค. ๋˜ํ•œ, ๋””์ ค ์—ฐ์†Œ๋กœ ์ธํ•œ ์งˆ์†Œ์‚ฐํ™”๋ฌผ๊ณผ ๊ทธ์„์Œ ๋ฐฐ์ถœ์€ ์ธ๊ฐ„์˜ ๊ฑด๊ฐ•์— ํ•ด๋กœ์šฐ๋ฉฐ ์ƒ๋ช…๊นŒ์ง€๋„ ์œ„ํ˜‘ํ•œ๋‹ค. ๋ฐฐ๊ธฐ ๊ฐ€์Šค์˜ ์œ ํ•ด์„ฑ์€ ๋งŽ์€ ๋‚˜๋ผ๋“ค์˜ ์ •๋ถ€๋“ค๋กœ ํ•˜์—ฌ๊ธˆ ์ฐจ๋Ÿ‰ ๋ฐฐ์ถœ ๊ทœ์ œ๋ฅผ ์—„๊ฒฉํ•˜๊ฒŒ ๋งŒ๋“ค๋„๋ก ๋™๊ธฐ๋ฅผ ๋ถ€์—ฌํ•˜๊ณ  ์žˆ๋‹ค. ์ตœ๊ทผ์—๋Š” ์‹คํ—˜์‹ค์˜ ์ธ์ฆ์น˜์™€ ๋„๋กœ์˜ ์‹ค์ œ ๋ฐฐ์ถœ๋Ÿ‰ ์ˆ˜์ค€ ๊ฐ„์˜ ์ฐจ์ด๋ฅผ ๊ณ ๋ คํ•ด Real-driving emissions ๊ทœ์ œ๊ฐ€ ์‹œํ–‰๋๋‹ค. ์†Œ์Œ ๊ณตํ•ด๋Š” ๋˜ํ•œ ์ธ๊ฐ„๊ณผ ๊ณต์ค‘ ๋ณด๊ฑด ๋ฌธ์ œ์˜ ๊ด€์ ์—์„œ ์ค‘์š”ํ•œ ์ฃผ์ œ์ด๋‹ค. ์—”์ง„์—์„œ ๋ฐœ์ƒํ•˜๋Š” ์—ฐ์†Œ ์†Œ์Œ์€ ์—”์ง„ ๋ณ€์ˆ˜ ๋ฐ ์—ฐ์†Œ ํŠน์„ฑ์— ์˜ํ•ด ์˜ํ–ฅ์„ ๋ฐ›๋Š” ์‹ค๋ฆฐ๋” ์••๋ ฅ ๋ฐฐ์ถœ์— ๋”ฐ๋ผ ๋‹ฌ๋ผ์ง„๋‹ค. ์ ์ ˆํ•œ ๋ถ„์‚ฌ ์ „๋žต ๋˜๋Š” ์—ฐ์†Œ ํ˜•ํƒœ๋Š” ์›ํ•˜๋Š” ์—ฐ์†Œ ์†Œ์Œ ์ˆ˜์ค€์„ ๋งŒ์กฑํ•˜๋„๋ก ์ตœ์ ํ™”ํ•  ์ˆ˜ ์žˆ๋‹ค. ์—”์ง„ ๊ฐœ๋ฐœ ๊ณผ์ • ์ค‘์— ์—ฐ๋น„, ๋ฐฐ๊ธฐ ๋ฐฐ์ถœ๋ฌผ ๋ฐ ์†Œ์Œ์˜ ๊ฐ ์„ฑ๋Šฅ์„ ์ตœ์ ํ™”ํ•˜๊ธฐ ์œ„ํ•œ ๋งŽ์€ ๋…ธ๋ ฅ๊ณผ ์‹œ๊ฐ„์ด ์†Œ๋ชจ๋œ๋‹ค. ์ตœ์ ์˜ ์„ฑ๋Šฅ์„ ์–ป์œผ๋ ค๋ฉด ์—ฐ์†Œ ๋ฐ ์—”์ง„ ์ž‘๋™ ๋ณ€์ˆ˜๋ฅผ ์ตœ์ ํ™”ํ•˜๊ธฐ ์œ„ํ•ด ๋งŽ์€ ์‹คํ—˜์ด ํ•„์š”ํ•˜๋‹ค. ์‹คํ—˜ ์—†์ด ์—”์ง„ ์„ฑ๋Šฅ์„ ์ตœ์ ํ™”ํ•˜๊ธฐ ์œ„ํ•ด ์ „์‚ฐ์œ ์ฒด์—ญํ•™ ์‹œ๋ฎฌ๋ ˆ์ด์…˜์„ ์ˆ˜ํ–‰ํ•˜๋ ค๋ฉด ๋†’์€ ๊ณ„์‚ฐ ๋น„์šฉ์ด ํ•„์š”ํ•˜๋‹ค. ๋”ฐ๋ผ์„œ, ๊ณ„์‚ฐ ๋น„์šฉ์ด ๋‚ฎ์€ 0-D ์—ฐ์†Œ ์ตœ์ ํ™” ๋ฐฉ๋ฒ•๋ก ์„ ๊ฐœ๋ฐœํ•˜๋Š” ๊ฒƒ์ด ์ค‘์š”ํ•˜๋‹ค. ์ด์ „ ์—ฐ๊ตฌ๋“ค์— ์˜ํ•œ 0-D ์—ฐ์†Œ ์ตœ์ ํ™” ๋ฐฉ๋ฒ•์€ ๋ถ„์‚ฌ ์ „๋žต ๋˜๋Š” ์—”์ง„ ๋ณ€์ˆ˜๋ฅผ ์ตœ์ ํ™”ํ–ˆ๋‹ค. ๊ฒฐ๊ณผ๋กœ ๋„์ถœ๋˜๋Š” ์—ฐ์†Œ๋Š” ๊ธฐ์กด ์—ฐ์†Œ ํ˜•์ƒ์˜ ๋ฒ”์œ„ ๋‚ด์— ์žˆ์œผ๋ฉฐ ์—ฐ์†Œ ํ˜•์ƒ์˜ ๋‹ค์–‘์„ฑ ์ธก๋ฉด์—์„œ ์‹คํ—˜์ ์œผ๋กœ ๋ณ€์ˆ˜๋ฅผ ์ตœ์ ํ™”ํ•˜๋Š” ๋ฐฉ๋ฒ•๊ณผ ๋‹ค๋ฅผ ๋ฐ” ์—†๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์›ํ•˜๋Š” ์„ฑ๋Šฅ์„ ์ž…๋ ฅ์œผ๋กœ, ์ตœ์  ์—ฐ์†Œ ๋ฐ ์—ฐ์†Œ ๋ณ€์ˆ˜๋ฅผ ์ถœ๋ ฅ์œผ๋กœ ๋„์ถœ๋˜๋Š” ์—ฐ์†Œ ๋””์ž์ธ ๋ฐฉ๋ฒ•๋ก ์„ ๊ฐœ๋ฐœํ•˜์˜€๋‹ค. ์ฒซ ๋ฒˆ์งธ ๋‹จ๊ณ„๋กœ ์—”์ง„ ์‹คํ—˜์„ ์ˆ˜ํ–‰ํ•˜์—ฌ ๋ฒ ์ด์Šค ์กฐ๊ฑด, EGR ์Šค์œ™, ํก๊ธฐ ์˜จ๋„ ๋ฐ ๋ƒ‰๊ฐ์ˆ˜ ์˜จ๋„ ์Šค์œ™ ์กฐ๊ฑด์—์„œ์˜ ์—ฐ๋น„ ๋ฐ ๋ฐฐ๊ธฐ ๋ฐฐ์ถœ์˜ ๊ธฐ๋ณธ ์„ฑ๋Šฅ์„ ํ‰๊ฐ€ํ•˜์˜€๋‹ค. ์ด ๊ฒฐ๊ณผ๋Š” ์—ฐ์†Œ ๋””์ž์ธ์— ํ™œ์šฉ๋˜๋Š” 0-D soot ๋ชจ๋ธ ์ˆ˜๋ฆฝ๊ณผ ์ตœ์ ํ™” ๊ณผ์ •์—์„œ ์ดˆ๊ธฐ ์กฐ๊ฑด์œผ๋กœ ์‚ฌ์šฉ๋˜์—ˆ๋‹ค. Soot ์ƒ์„ฑ ๋ชจ๋ธ์€ lift-off length์—์„œ ๋‹น๋Ÿ‰๋น„๋ฅผ ๊ณ„์‚ฐํ•˜๋Š” ๋‹จ์ˆœํ™”๋œ ์Šคํ”„๋ ˆ์ด ๋ชจ๋ธ์„ ๊ธฐ๋ฐ˜์œผ๋กœ ํ–ˆ๋‹ค. Lift-off length์—์„œ์˜ ๋‹น๋Ÿ‰๋น„๋Š” ๊ทธ์„์Œ ํ˜•์„ฑ ๋ชจ๋ธ์˜ ์ฃผ์š” ์š”์ธ ์ค‘ ํ•˜๋‚˜๋กœ ์‚ฌ์šฉ๋˜์—ˆ๋‹ค. ์—ฐ์†Œ ๋””์ž์ธ ๊ณผ์ •์—์„œ IMEP๋Š” ์—ฐ๋น„๋ฅผ ๋Œ€๋ณ€ํ•˜๋Š” ์ธ์ž๋กœ ์‚ฌ์šฉ๋˜์—ˆ๋‹ค. ์—ฐ์†Œ ์†Œ์Œ ํ‰๊ฐ€์—๋Š” ์—ฐ์†Œ ์†Œ์Œ ์ง€์ˆ˜๊ฐ€ ์‚ฌ์šฉ๋˜์—ˆ๋‹ค. NOx ๋ฐฐ์ถœ๋Ÿ‰ ์˜ˆ์ธก์—๋Š” ์ด์ „ ์—ฐ๊ตฌ๋กœ๋ถ€ํ„ฐ ๊ฐœ๋ฐœ๋œ 0-D NOx ๋ชจ๋ธ์ด ์ ์šฉ๋˜์—ˆ๋‹ค. ์—ฐ์†Œ ๋””์ž์ธ ๋ฐฉ๋ฒ•๋ก ์—์„œ, ์‹ค๋ฆฐ๋” ๋‚ด ์••๋ ฅ ๊ณ„์‚ฐ์— ํ•„์š”ํ•œ ๋ณ€์ˆ˜๋Š” ํก๊ธฐ ์••๋ ฅ, ๋žŒ๋‹ค ๋ฐ ์งˆ๋Ÿ‰ ์—ฐ์†Œ์œจ์ด์—ˆ๋‹ค. ์งˆ๋Ÿ‰ ์—ฐ์†Œ์œจ์€ ๊ธฐ์กด์— ๋„๋ฆฌ ์‚ฌ์šฉ๋˜๋Š” ์œ„๋ฒ  ํ•จ์ˆ˜์™€ ์—ฐ์†Œ์ƒ์— ๋Œ€ํ•œ ์ƒˆ๋กœ์šด ์ ‘๊ทผ๋ฒ•์œผ๋กœ ๋‹คํ•ญ์‹ ํ•จ์ˆ˜๋ฅผ ์‚ฌ์šฉํ•˜์—ฌ ๊ฒฐ์ •๋˜์—ˆ๋‹ค. ์‹ค๋ฆฐ๋” ๋‚ด ๊ณต๊ธฐ์˜ ์งˆ๋Ÿ‰๊ณผ EGR์œจ์€ ์ดˆ๊ธฐ ์กฐ๊ฑด์œผ๋กœ ๊ฒฐ์ •๋œ ํก๊ธฐ ์••๋ ฅ, ์˜จ๋„, ๋žŒ๋‹ค ๋ฐ ํ™”ํ•™ ๋ฐ˜์‘ ๋ฐฉ์ •์‹์œผ๋กœ ๊ณ„์‚ฐ๋˜์—ˆ๋‹ค. ์—ฐ์†Œ ์ค‘์˜ ๊ธฐ์ฒด ์กฐ์„ฑ๋น„๋Š” polytropic ์ง€์ˆ˜ ๋ฐ ์—ฌ๋Ÿฌ ์—ด์—ญํ•™์  ๋ณ€์ˆ˜์˜ ๊ณ„์‚ฐ์„ ์œ„ํ•ด ๊ณ„์‚ฐ๋˜์—ˆ๋‹ค. ์‹ค๋ฆฐ๋” ๋‚ด ์••๋ ฅ์€ polytropic ๊ณผ์ •๊ณผ ์—ด ๋ฐœ์ƒ๋ฅ ์œผ๋กœ ๊ณ„์‚ฐ๋˜์—ˆ๋‹ค. ์ตœ์ ํ™” ๊ณผ์ •์—์„œ ์—ฐ์†Œ ๋””์ž์ธ ๋ฐฉ๋ฒ•์— ์‚ฌ์šฉ๋œ ์ตœ์ ํ™” ์•Œ๊ณ ๋ฆฌ์ฆ˜์€ ์ œํ•œ๋œ ๋น„์„ ํ˜• ๋‹ค๋ณ€๋Ÿ‰ ํ•จ์ˆ˜(Interior-point ๊ธฐ๋ฒ•)์™€ ์ž…์ž ๊ตฐ์ง‘ ์ตœ์ ํ™”์˜ ์ตœ์†Œ๊ฐ’์ด์—ˆ๋‹ค. ๊ฒฝ๊ณ„ ์กฐ๊ฑด๊ณผ ์ œ์•ฝ ์กฐ๊ฑด์€ ์ตœ์ ํ™” ๊ณผ์ •์˜ ํšจ์œจ์ ์ธ iteration์„ ์œ„ํ•ด ๊ฒฐ์ •๋˜์—ˆ๋‹ค. ์ตœ์ ํ™”๋ฅผ ์œ„ํ•œ ๋ชฉ์  ํ•จ์ˆ˜์˜ ๊ธฐ๋ณธ ํ˜•ํƒœ๋Š” ์ž…๋ ฅ์œผ๋กœ ์‚ฌ์šฉ๋œ ์›ํ•˜๋Š” ์„ฑ๋Šฅ์„ ๊ฐ€์ง€๋Š” ํŠน์ •ํ•œ ์—ฐ์†Œ๋ฅผ ์ฐพ์„ ์ˆ˜ ์žˆ๊ฒŒ ํ–ˆ๋‹ค. ๋ชฉํ‘œ ์„ฑ๋Šฅ์„ ์ตœ๋Œ€ํ™”ํ•˜๋Š” ๋‹ค์–‘ํ•œ ๋””์ž์ธ ๋ชฉ์ ์— ๋”ฐ๋ผ ๋ชฉํ‘œ ํ•จ์ˆ˜๋Š” ๋ณ€ํ˜•๋˜์–ด ์‚ฌ์šฉ๋˜์—ˆ๋‹ค. ์—ฐ์†Œ ๋””์ž์ธ์˜ ๊ฒฐ๊ณผ๋Š” ๋‹ค์–‘ํ•œ ์šด์ „ ์˜์—ญ์—์„œ MFB์™€ ๋ชฉ์  ํ•จ์ˆ˜์— ๋”ฐ๋ผ ์—ฐ๊ตฌ๋˜์—ˆ๋‹ค. WLTP ์šด์ „ ์˜์—ญ์—์„œ ์ •์ƒ ์ƒํƒœ ์—ฐ์†Œ๋“ค์„ ๋””์ž์ธํ•˜์—ฌ ์—ฐ์†Œ ๋””์ž์ธ ๋ฐฉ๋ฒ•๋ก ์„ WLTP์— ์ ์šฉํ•˜์˜€๋‹ค. ์ ์šฉ ๊ฒฐ๊ณผ, WLTP ์ค‘ ์—ฐ๋ฃŒ ์†Œ๋ชจ๋Ÿ‰์€ 4.7% ๊ฐ์†Œ๋˜์—ˆ๋‹ค. NOx์™€ soot ๋ฐฐ์ถœ์€ ๊ฐ๊ฐ 44.7%์™€ 60.7%์˜ ๊ฐ์†Œ์œจ์„ ๋ณด์˜€๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์›ํ•˜๋Š” ์„ฑ๋Šฅ์˜ ์—ฐ์†Œ๋ฅผ ๋„์ถœํ•˜๋Š” 0-D ์—ฐ์†Œ ์‹œ๋ฎฌ๋ ˆ์ด์…˜ ๋ฐ ์ตœ์ ํ™” ๋ฐฉ๋ฒ•์„ ์ œ๊ณตํ•˜์˜€๋‹ค. ์ด ์—ฐ๊ตฌ๋Š” ์›ํ•˜๋Š” ์„ฑ๋Šฅ ํ˜น์€ ์ตœ์ ํ™”๋œ ์„ฑ๋Šฅ์„ ๊ฐ€์ง€๋Š” ์—ฐ์†Œ์ƒ์„ ์—ด์—ญํ•™์ ์ธ ์กฐ๊ฑด๋“ค๊ณผ ํ•จ๊ป˜ ์ œ์‹œํ•  ์ˆ˜ ์žˆ์–ด ์ด๋ฅผ ๋ฐ”ํƒ•์œผ๋กœ ๊ธฐ์กด์˜ ์—ฐ๊ตฌ ๋ฐฉ๋ฒ•๊ณผ ๋‹ค๋ฅธ ๋ชฉํ‘œ ์—ฐ์†Œ๋ฅผ ๊ตฌํ˜„ํ•˜๊ธฐ ์œ„ํ•œ ์—”์ง„๊ณผ ์—ฐ์†Œ ์ „๋žต ๊ฐœ๋ฐœ ๋ฐฉํ–ฅ์„ ์ œ์‹œํ•  ์ˆ˜ ์žˆ๋‹ค.Recently, the researches for improving the performance of the internal combustion engines have been focused on the respect of thermal efficiency, emissions, noise and vibration. The thermal efficiency is related with decreasing carbon dioxide (CO2) emission that has affected global warming. Also, nitrogen oxides (NOx) and soot emissions from diesel combustion are harmful for human. The harmfulness of exhaust gases has motivated governments of many countries to make vehicle emission regulations stringent. Recently, real-driving emissions (RDE) regulation was enforced, considering the discrepancy between the certified values in laboratory and the actual emission levels on the road. Noise pollution is also important in the perspective of human and public health problem. The combustion noise from the engine depends on the cylinder pressure excitation, which is affected by the engine parameters and combustion characteristics. Proper injection strategies or combustion shape can be optimized to meet the desired combustion noise level. The engine development process takes a lot of effort and time to optimize each performance of thermal efficiency, emissions and noise. To achieve desired optimal performance, many trials and errors and experiments are required to optimize combustion and engine operating parameters. As an optimization tool, computational fluid dynamics (CFD) simulation needs substantial calculation cost. Thus, it is important to develop 0-D combustion optimization methodology that has low calculation cost. Previously studied 0-D combustion optimization methods have been optimized the injection strategy or engine parameters. The resulting combustion comes out of a narrow range and it is similar to the methodology of optimizing variables experimentally in terms of diversity of combustion. In this study, the combustion design methodology was developed that used the desired performance as input and derived combustion and combustion parameters as outputs in a diesel engine. The thermal efficiency, noise and emissions were needed to be calculated by 0-D combustion simulation for the combustion optimization. As a one of emission models, the 0-D soot model was developed through cooperative research with Youngbok Lee. The engine test that evaluated the soot emission by EGR rate, intake and coolant temperature was conducted to develop the 0-D soot model and acquire initial conditions for combustion design. The soot formation model was based on the simplified spray model to calculate the equivalence ratio at lift-off length. The equivalence ratio at the lift-off length was used as a one of the main factor for the soot formation model. In the combustion design process, IMEP represented the thermal efficiency. For the combustion noise evaluation, the combustion noise index was used. The 0-D NOx model from previous research was applied to estimate NOx emission. In the combustion design methodology, the initial parameters for constructing in-cylinder pressure were intake pressure, lambda and the mass faction burned. The MFB was determined by using Wiebe function and polynomial function as new approach to combustion phase. The mass of in-cylinder air and EGR rate were calculated from intake pressure, temperature, lambda, that were determined as initial conditions, and the chemical reaction equation. Compression and expansion strokes were assumed as polytropic process. The gas compositions during the combustion were calculated for calculation of polytropic index and other thermodynamic parameters. The in-cylinder pressure was calculated by the heat release rate and polytropic process with the estimated polytropic index. In the optimization process, the optimization algorithms used in the combustion design method were a minimum of constrained nonlinear multivariable function (interior-point) and particle swarm optimization. MATLAB was used as the optimization tool. The boundary conditions and constraints were determined for efficient iteration in optimization process. The base form of objective function for optimization allowed to find specific combustion of desired performance that was used as input. The objective functions for various design concepts were used in maximizing target performance. The results of combustion design were investigated by objective function and MFB function type at various operation point. The combustion design method was applied to WLTP by designing the steady points in WLTP operation region. The fuel consumption during WLTP decreased by 4.6% compared to experimental result The NOx and soot emissions could be reduced by 44.7% and 60.7%. In this study, the 0-D combustion simulation and optimization method that derived the combustion of desired performance were provided. This research can contribute to provide combustion shape with desired or optimized performance in combination with thermodynamic conditions, suggesting the development process different from existing research methods of engine and combustion strategies for target combustion.Chapter 1. Introduction 1 1.1 Background 1 1.2 Literature Review 8 1.2.1 Combustion noise model 8 1.2.2 NOx emission model 11 1.2.3 Soot emission model 13 1.2.4 Combustion optimization 18 1.3 Research Objectives and Contributions 28 1.4 Structure of the Thesis 29 Chapter 2. Experimental Apparatus 31 2.1 Experimental Setup 31 2.1.1 Test engine 31 2.1.2 Test cell and data acquisition systems 31 2.1.3 Emission measurement systems 32 2.1.4 Engine operating conditions 34 Chapter 3. Semi-physical 0-D Soot Model 46 3.1 Simplified Spray Model 46 3.1.1 Spray model description 46 3.1.2 Liquid length calculation 48 3.1.3 Laminar flame speed model 50 3.1.4 The equivalence ratio at the lift-off length 53 3.2 Semi-physical 0-D Soot Model 64 3.2.1 Soot formation model 64 3.2.2 Soot oxidation model 65 3.2.3 The model validation 68 Chapter 4. Other Models for Thermal Efficiency, Noise and NOx Emission 74 4.1 Thermal Efficiency 74 4.2 Noise โ€“ Combustion Noise Index (CNI) 74 4.3 The NOx Estimation Model 78 Chapter 5. Combustion Design Methodology 81 5.1 Concept of Combustion Design Method 81 5.2 Process of Constructing Combustion Pressure 86 5.2.1 Mass fraction burned and heat release rate 86 5.2.2 Calculation of in-cylinder air flow and EGR rate 95 5.2.3 Gas composition during the combustion process 102 5.2.4 Polytropic index and constructing cylinder pressure 103 5.2.5 Calculation of the fuel injection timing 107 5.3 Optimization Methodology 113 5.3.1 Optimization algorithms 113 5.3.2 Boundary conditions and constraints 116 5.3.3 Determination of the objective function 121 Chapter 6. Results of Combustion Design 131 6.1 Results from Base Objective Function 131 6.1.1 Low load: 1500 rpm, BMEP 4 bar 131 6.1.2 High load: 2000 rpm, BMEP 8 bar 136 6.2 Results by various design concept 141 6.3 Results Using Polynomial Function as MFB 148 6.4 Application of Combustion Design to WLTP 153 6.4.1 Combustion design at steady points in WLTP operating area 153 6.4.2 Results of an application to WLTP 164 Chapter 7. Conclusions 169 Bibliography 174 ๊ตญ ๋ฌธ ์ดˆ ๋ก 193๋ฐ•

    Development of Automated Calibration Methodology for Last Generation of Diesel Automotive Powertrains

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    L'abstract รจ presente nell'allegato / the abstract is in the attachmen

    Non-weighted aggregate evaluation function of multi-objective optimization for knock engine modeling

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    In decision theory, the weighted sum model (WSM) is the best known Multi-Criteria Decision Analysis (MCDA) approach for evaluating a number of alternatives in terms of a number of decision criteria. Assigning weights is a difficult task, especially if the number of criteria is large and the criteria are very different in character. There are some problems in the real world which utilize conflicting criteria and mutual effect. In the field of automotive, the knocking phenomenon in internal combustion or spark ignition engines limits the efficiency of the engine. Power and fuel economy can be maximized by optimizing some factors that affect the knocking phenomenon, such as temperature, throttle position sensor, spark ignition timing, and revolution per minute. Detecting knocks and controlling the above factors or criteria may allow the engine to run at the best power and fuel economy. The best decision must arise from selecting the optimum trade-off within the above criteria. The main objective of this study was to proposed a new Non-Weighted Aggregate Evaluation Function (NWAEF) model for non-linear multi-objectives function which will simulate the engine knock behavior (non-linear dependent variable) in order to optimize non-linear decision factors (non-linear independent variables). This study has focused on the construction of a NWAEF model by using a curve fitting technique and partial derivatives. It also aims to optimize the nonlinear nature of the factors by using Genetic Algorithm (GA) as well as investigate the behavior of such function. This study assumes that a partial and mutual influence between factors is required before such factors can be optimized. The Akaike Information Criterion (AIC) is used to balance the complexity of the model and the data loss, which can help assess the range of the tested models and choose the best ones. Some statistical tools are also used in this thesis to assess and identify the most powerful explanation in the model. The first derivative is used to simplify the form of evaluation function. The NWAEF model was compared to Random Weights Genetic Algorithm (RWGA) model by using five data sets taken from different internal combustion engines. There was a relatively large variation in elapsed time to get to the best solution between the two model. Experimental results in application aspect (Internal combustion engines) show that the new model participates in decreasing the elapsed time. This research provides a form of knock control within the subspace that can enhance the efficiency and performance of the engine, improve fuel economy, and reduce regulated emissions and pollution. Combined with new concepts in the engine design, this model can be used for improving the control strategies and providing accurate information to the Engine Control Unit (ECU), which will control the knock faster and ensure the perfect condition of the engine

    ๊ฐ€์†”๋ฆฐ ์—”์ง„์—์„œ์˜ 0-D ๋…ธํ‚น ๋ฐœ์ƒ์˜ˆ์ธก ๋ชจ๋ธ๋ง์— ๊ด€ํ•œ ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ (์„์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€, 2019. 2. ๋ฏผ๊ฒฝ๋•.๊ฐ€์†”๋ฆฐ ์—”์ง„์˜ ํšจ์œจ ํ–ฅ์ƒ์€ ์ง€์†์ ์œผ๋กœ ์—ฐ๊ตฌ๋˜์–ด ์™”์œผ๋‚˜, ์ตœ๊ทผ์˜ ๊ธ‰๊ฒฉํžˆ ๊ฐ•ํ™”๋˜๋Š” ์—ฐ๋น„, ๋ฐฐ๊ธฐ ๊ทœ์ œ๋กœ ์ธํ•ด ํšจ์œจ ํ–ฅ์ƒ์˜ ํ•„์š”์„ฑ์ด ๊ทธ ์–ด๋Š ๋•Œ๋ณด๋‹ค ๋”์šฑ ๋Œ€๋‘๋˜๊ณ  ์žˆ๋‹ค. ๋”ฐ๋ผ์„œ ๊ฐ€์†”๋ฆฐ ์—”์ง„์˜ ํšจ์œจ ํ–ฅ์ƒ์„ ์œ„ํ•œ ๋‹ค์–‘ํ•œ ๋ฐฉ๋ฒ•์ด ์ œ์‹œ๋˜๊ณ  ์žˆ์œผ๋ฉฐ, ๊ทธ ์ค‘์—์„œ๋„ ์••์ถ•๋น„์˜ ์ƒ์Šน์€ ํšจ์œจ ๊ฐœ์„ ์— ๋งค์šฐ ํšจ๊ณผ์ ์ด๋‹ค. ๊ทธ๋Ÿฌ๋‚˜ ์••์ถ•๋น„์˜ ์ƒ์Šน์€ ํ˜ผํ•ฉ๊ธฐ์˜ ์ดˆ๊ธฐ ์˜จ๋„๋ฅผ ์ƒ์Šน์‹œํ‚ค๋ฉฐ, ์ด๋Š” ์—ฐ์†Œ๊ธฐ๊ฐ„ ์ค‘ ๋ง๋‹จ๊ฐ€์Šค์˜ ์˜จ๋„ ์ƒ์Šน์œผ๋กœ ์ง๊ฒฐ๋˜์–ด ๋ฏธ์—ฐ ๊ฐ€์Šค์˜ ์ž๋ฐœํ™” ํ˜„์ƒ์ด ๋ฐœ์ƒํ•˜๊ธฐ ์‰ฝ๊ฒŒ ํ•œ๋‹ค. ์ž๋ฐœํ™” ํ˜„์ƒ์ด ํญ๋ฐœ์˜ ํ˜•ํƒœ๋กœ ๋ฐœ์ƒํ•˜๋Š” ๊ฒฝ์šฐ, ์ˆœ๊ฐ„์ ์ธ ์—ด ๋ฐฉ์ถœ์ด ๋ฐœ์ƒํ•˜๊ณ  ์‹ค๋ฆฐ๋” ๋‚ด๋ถ€์— ์••๋ ฅํŒŒ๋ฅผ ํ˜•์„ฑํ•˜์—ฌ ์†Œ์Œ๊ณผ ์—”์ง„ ์†์ƒ์„ ์œ ๋ฐœํ•œ๋‹ค. ์ด๋Š” ๋…ธํ‚น ํ˜„์ƒ์œผ๋กœ ๋ถˆ๋ฆฌ๋ฉฐ, ์—”์ง„ ์†์ƒ์„ ๋ฐฉ์ง€ํ•˜๊ธฐ ์œ„ํ•˜์—ฌ ๋ฐ˜๋“œ์‹œ ํšŒํ”ผ๋˜์–ด์•ผ ํ•œ๋‹ค. ๋”ฐ๋ผ์„œ ์ด์— ๋Œ€ํ•ด ๋…ธํ‚น์„ ์ €๊ฐํ•˜๋Š” ์—ฐ๊ตฌ๋ฟ๋งŒ ์•„๋‹ˆ๋ผ, ๋…ธํ‚น์„ ํšŒํ”ผํ•˜๊ธฐ ์œ„ํ•œ ๋‹ค์–‘ํ•œ ์ œ์–ด ์•Œ๊ณ ๋ฆฌ์ฆ˜์ด ์ œ์‹œ๋˜๊ณ  ์žˆ๋‹ค. ๊ธฐ์กด ์–‘์‚ฐ ์ฐจ๋Ÿ‰์—์„œ์˜ ๋…ธํ‚น ์ œ์–ด ์•Œ๊ณ ๋ฆฌ์ฆ˜์€ ๋…ธํ‚น ์„ผ์„œ์— ์˜์กดํ•˜๊ณ  ์žˆ์œผ๋ฉฐ, ์ด๋Š” ์„ผ์„œ์—์„œ ๋…ธํ‚น ๋ฐœ์ƒ์„ ๊ฐ์ง€ํ•˜๋Š” ๊ฒƒ์ด ์„ ํ–‰๋˜์–ด์•ผ ํ•˜๋ฏ€๋กœ ๋…ธํ‚น์„ ์™„์ „ํžˆ ํšŒํ”ผํ•  ์ˆ˜ ์—†๋‹ค. ๋˜ํ•œ, ๋…ธํ‚น ๋ฐœ์ƒ ์‹œ ํšŒํ”ผ๋ฅผ ์œ„ํ•ด ์ œ์–ด์ธ์ž๊ฐ€ ๊ธ‰๊ฒฉํžˆ ๋ณ€๊ฒฝ๋˜๋ฉฐ, ์ด๋Š” ์šด์ „ํŽธ์˜์„ฑ์ด ๋‚˜๋น ์งˆ ๋ฟ๋งŒ ์•„๋‹ˆ๋ผ, ์—”์ง„ ํšจ์œจ์„ ๊ฐ์†Œ์‹œํ‚ค๊ฒŒ ๋œ๋‹ค. ์ด๋Ÿฌํ•œ ์ ์„ ๊ฐœ์„ ํ•˜๊ธฐ ์œ„ํ•ด ์ œ์–ด์ธ์ž๋ฅผ ์ ์ง„์ ์œผ๋กœ ๋ณ€๊ฒฝํ•˜๋Š” ๋“ฑ ์ง„๋ณด์ ์ธ ์ œ์–ด ๋ฐฉ๋ฒ•์ด ๊ฐœ๋ฐœ๋˜๊ณ  ์žˆ๋‹ค. ๋…ธํ‚นํ˜„์ƒ์€ ์—”์ง„ ๋‚ด์˜ ์œ ๋™, ์—ด ์ „๋‹ฌ ๋ฐ ์—ฐ์†Œ ํŠน์„ฑ๊ณผ ๊ฐ™์€ ์ธ์ž์— ์˜ํ–ฅ์„ ๋ฐ›์œผ๋ฏ€๋กœ, ๋ฌด์ž‘์œ„์ ์ธ ํŠน์„ฑ์„ ๋ณด์ธ๋‹ค. ๋”ฐ๋ผ์„œ, ๋…ธํ‚น์„ ๋ณด์ˆ˜์ ์œผ๋กœ ํšŒํ”ผํ•˜๊ธฐ ์œ„ํ•ด ๊ธฐ์กด์˜ ์ œ์–ด๋Š” ๋…ธํ‚น ํšŒํ”ผ ํ›„์— ์šด์ „ ์ธ์ž๋ฅผ ์ฒœ์ฒœํžˆ ์ตœ์  ์šด์ „ ์กฐ๊ฑด์œผ๋กœ ๋ณต๊ท€์‹œํ‚จ๋‹ค. ์ด๋Š” ์ „๋ฐ˜์ ์œผ๋กœ ํšจ์œจ์ด ๋‚ฎ์€ ์ง€์ ์— ์šด์ „ ์กฐ๊ฑด์„ ์œ ์ง€์‹œํ‚ค๋ฏ€๋กœ, ์ด๋ฅผ ๊ฐœ์„ ํ•œ๋‹ค๋ฉด ๊ณ ๋ถ€ํ•˜ ์กฐ๊ฑด์—์„œ ์ถ”๊ฐ€์ ์ธ ํšจ์œจ ์ƒ์Šน์„ ๊ธฐ๋Œ€ํ•  ์ˆ˜ ์žˆ๋‹ค. ์ด์— ๋Œ€ํ•œ ๊ฐœ์„  ๋ฐฉ๋ฒ•์˜ ํ•˜๋‚˜๋กœ ๋…ธํ‚น์„ ์˜ˆ์ธกํ•˜์—ฌ ์„ ์žฌ์ ์œผ๋กœ ์ œ์–ด๋ฅผ ์ˆ˜ํ–‰ํ•˜๋Š” ๋ชจ๋ธ ๊ธฐ๋ฐ˜์˜ ์ œ์–ด๋ฅผ ์ œ์‹œํ•  ์ˆ˜ ์žˆ๋‹ค. ์ด ๊ฒฝ์šฐ, ๋…ธํ‚น์„ ํšŒํ”ผํ•˜๊ธฐ ์šฉ์ดํ•ด ์งˆ ๋ฟ๋งŒ ์•„๋‹ˆ๋ผ, ๋…ธํ‚น ๋ฐœ์ƒ ์‚ฌ์ „์— ์ œ์–ด ์ธ์ž๋ฅผ ์ง€์ •ํ•จ์œผ๋กœ์จ ๊ธฐ์กด์— ๋ฐœ์ƒํ•˜๋˜ ๊ณผ๋„ํ•œ ์ œ์–ด ์ธ์ž ๋ณ€๊ฒฝ์œผ๋กœ ์ธํ•œ ํšจ์œจ ์ €ํ•˜๋ฅผ ๋ฐฉ์ง€ํ•  ์ˆ˜ ์žˆ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์„ ์žฌ์  ์ œ์–ด๋ฅผ ์œ„ํ•œ ๊ธฐ์ €์—ฐ๊ตฌ๋กœ, ์—”์ง„์—์„œ์˜ ๋…ธํ‚น ๋ฐœ์ƒ ์˜ˆ์ธก์— ๋Œ€ํ•œ ๋ชจ๋ธ๋ง์ด ์ด๋ฃจ์–ด์กŒ๋‹ค. ๋ชจ๋ธ์—๋Š” ์‹ค์ œ ์šด์ „ ์ƒํ™ฉ์—์˜ ์ ์šฉ์„ ๊ณ ๋ คํ•˜์—ฌ, ๊ธฐ์กด ์–‘์‚ฐ ์—”์ง„์—์„œ ์–ป์„ ์ˆ˜ ์žˆ๋Š” ๋ณ€์ˆ˜ ๋ฐ ์ธก์ •๊ฐ’๋งŒ์ด ์ด์šฉ๋˜์—ˆ๋‹ค. ์ฒซ์งธ๋กœ, ์‹ค๋ฆฐ๋” ๋‚ด ์••๋ ฅ ์˜ˆ์ธก ๋ชจ๋ธ๋ง์ด ์ด๋ฃจ์–ด ์กŒ์œผ๋ฉฐ, ์ด๋Š” ์‹ค๋ฆฐ๋” ๋‚ด๋ถ€ ์ดˆ๊ธฐ ์กฐ๊ฑด์˜ ํŒ์ •, ์••์ถ•๊ธฐ๊ฐ„ ๋™์•ˆ์˜ ์••๋ ฅ ์˜ˆ์ธก, ๊ทธ๋ฆฌ๊ณ  ์—ฐ์†Œ์œจ์„ ์ด์šฉํ•œ ์—ฐ์†Œ ์••๋ ฅ ์˜ˆ์ธก์˜ ์„ธ๊ฐ€์ง€ ๊ณผ์ •์œผ๋กœ ์ง„ํ–‰๋˜์—ˆ๋‹ค. ๋‘˜์งธ๋กœ, ์˜ˆ์ธก๋œ ์••๋ ฅ์„ ์ด์šฉํ•˜์—ฌ ๋ฏธ์—ฐ๊ฐ€์Šค์˜ ์˜จ๋„๋ฅผ ๊ณ„์‚ฐํ•˜์˜€์œผ๋ฉฐ, ์ด๋Š” ์ ํ™” ์ง€์—ฐ์„ ๊ณ„์‚ฐํ•˜๋Š” ๋ฐ์— ์ด์šฉ๋˜์—ˆ๋‹ค. ์ ํ™” ์ง€์—ฐ์€ ์‹ค์ œ ์ž๋ฐœํ™” ๋ฐœ์ƒ ์—ฌ๋ถ€๋ฅผ ํŒ์ •ํ•˜์ง€ ๋ชปํ•˜๋ฏ€๋กœ, ์˜ˆ์ธก๋œ ์ž๋ฐœํ™” ์‹œ์ ์—์„œ์˜ ์—ฐ์†Œ์œจ์„ ์ด์šฉํ•˜์—ฌ ๋…ธํ‚น ์—ฌ๋ถ€๋ฅผ ํŒ์ •ํ•˜์˜€๋‹ค. ๊ตฌ์„ฑ๋œ ๋ชจ๋ธ์€ ์‚ฌ์ดํด ๋ณ„ ํŽธ์ฐจ๊ฐ€ ๊ณ ๋ ค๋œ ์••๋ ฅ ์˜ˆ์ธก๋ชจ๋ธ๊ณผ ํ•จ๊ป˜ ์ ์šฉ๋˜์—ˆ์„ ๊ฒฝ์šฐ ๋…ธํ‚น ๋ฐœ์ƒ ๋นˆ๋„๋ฅผ ์ž˜ ์˜ˆ์ธกํ•˜์—ฌ, ์ถฉ๋ถ„ํ•œ ์˜ˆ์ธก ์ •ํ™•์„ฑ์„ ๊ฐ€์ง€๊ณ  ์žˆ๋‹ค๊ณ  ํŒ๋‹จ๋˜์—ˆ๋‹ค.Though the efficiency improvements of gasoline engines have been continually studied, the recent surge in fuel efficiency and emissions regulations has made the need for greater effort on efficiency improvement than ever before. Therefore, various methods have been proposed to improve the efficiency of gasoline engines, and among them, the increase in compression ratio has been known to be effective in improving fuel efficiency. However, the higher compression ratio increases the initial temperature of the mixture, which is led to in-cylinder condition which auto-ignition is likely to occur. If auto-ignition occurs in the form of an explosion, a stiff heat release occurs and forms a pressure wave inside the cylinder, causing noise and engine damage. This is called a knock and must be avoided to prevent engine damage. Therefore, various control algorithms have been proposed to avoid knock as well as researches to mitigate knock. Knocking control algorithms in conventional mass-produced vehicles rely on knock sensors. Because it is preceded by detection of knock from sensors, knock cannot be completely avoided. In addition, the control parameters change rapidly to avoid convolutions in case of knock, which not only deteriorates the driving convenience but also decreases fuel efficiency In order to improve this point, progressive control methods are being developed. The knock phenomenon is influenced by factors such as gas flow, heat transfer and combustion characteristics in the engine, so that it shows random characteristics. Therefore, in order to avoid the knocking conservatively, the conventional control slowly returns the operating parameters to the optimum condition after knocking avoidance. This maintains the operating conditions at lower efficiency points, so additional efficiency improvement is expected in high load condition if the control algorithm is improved. As one of the solutions, an advanced control with knock prediction can be suggested. In this case, not only is it able to avoid knock, but also by determining control factors prior to knock occurrence, it is also possible to avoid efficiency deterioration due to excessive change in control parameters. In this study, modeling of knock prediction was done as a base study for model based control. In the model, only operating parameters and measured values obtainable from the mass production engine were used, considering the application to actual driving conditions. Firstly, the in-cylinder pressure prediction modeling was done with three stepsdetermination of the initial conditions inside the cylinder, pressure prediction during the compression, and combustion pressure prediction using the burn rate. Additionally, with consideration on variation of Wiebe function, the cyclic variation model was constructed. Secondly, the temperature of the unburned gas was calculated using the predicted pressure. With those value, the ignition delay was calculated. Since the ignition delay only determines the onset of auto-ignition, not the occurrence, the burn rate at predicted onset was used to determine the knock occurrence. The pressure prediction and ignition delay model were combined to a single model and tested with cyclic variation model. As a result, the model was judged to have sufficient accuracy, predicting knock incidence accurately under various operating conditions.Abstract i Contents iv List of Tables vi List of Figures vii Nomenclature ix Chapter 1. Introduction 1 1.1 Backgrounds and Motivations 1 1.2 Literature Review 6 1.2.1 Auto-ignition and knock phenomenon 6 1.2.2 Knock methodologies 10 1.2.3 Knock mitigation strategies 16 1.3 Research objective 20 Chapter 2. Methodology 21 2.1 Test cell configuration 21 2.1.1 Test engine specification 21 2.1.2 Cell facility and equipment 21 2.2 Experimental conditions 26 2.2.1 Knock detection and incidence 26 2.2.2 Operating condition 26 2.3 Combustion analysis 29 2.3.1 Heat release rate and heat loss 29 2.3.2 Knock onset determination 33 2.3.3 Unburned gas temperature 36 2.3.4 Residual gas fraction estimation 37 Chapter 3. Model Description 44 3.1 Prediction of in-cylinder pressure 44 3.1.1 Initial gas state 44 3.1.2 Compression process with polytropic index model 46 3.1.3 Combustion process estimation 50 3.1.4 Simulation of cyclic variation 57 3.2 Criteria for knock determination 60 3.2.1 Ignition delay estimation 60 3.2.2 Mass burned fraction and knock onset 63 Chapter 4. Result and discussion 65 Chapter 5. Conclusion 70 Bibliography 73 ๊ตญ ๋ฌธ ์ดˆ ๋ก 82Maste

    Optimization of adaptive test design methods for the determination of steady-state data-driven models in terms of combustion engine calibration

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    This thesis deals with the development of a model-based adaptive test design strategy with a focus on steady-state combustion engine calibration. The first research topic investigates the question how to handle limits in the input domain during an adaptive test design procedure. The second area of scope aims at identifying the test design method providing the best model quality improvement in terms of overall model prediction error. To consider restricted areas in the input domain, a convex hull-based solution involving a convex cone algorithm is developed, the outcome of which serves as a boundary model for a test point search. A solution is derived to enable the application of the boundary model to high-dimensional problems without calculating the exact convex hull and cones. Furthermore, different data-driven engine modeling methods are compared, resulting in the Gaussian process model as the most suitable one for a model-based calibration. To determine an appropriate test design method for a Gaussian process model application, two new strategies are developed and compared to state-of-the-art methods. A simulation-based study shows the most benefit applying a modified mutual information test design, followed by a newly developed relevance-based test design with less computational effort. The boundary model and the relevance-based test design are integrated into a multicriterial test design strategy that is tailored to match the requirements of combustion engine test bench measurements. A simulation-based study with seven and nine input parameters and four outputs each offered an average model quality improvement of 36 % and an average measured input area volume increase of 65 % compared to a non-adaptive space-filling test design. The multicriterial test design was applied to a test bench measurement with seven inputs for verification. Compared to a space-filling test design measurement, the improvement could be confirmed with an average model quality increase of 17 % over eight outputs and a 34 % larger measured input area

    ADAPTIVE MODEL BASED COMBUSTION PHASING CONTROL FOR MULTI FUEL SPARK IGNITION ENGINES

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    This research describes a physics-based control-oriented feed-forward model, combined with cylinder pressure feedback, to regulate combustion phasing in a spark-ignition engine operating on an unknown mix of fuels. This research may help enable internal combustion engines that are capable of on-the-fly adaptation to a wide range of fuels. These engines could; (1) facilitate a reduction in bio-fuel processing, (2) encourage locally-appropriate bio-fuels to reduce transportation, (3) allow new fuel formulations to enter the market with minimal infrastructure, and (4) enable engine adaptation to pump-to-pump fuel variations. These outcomes will help make bio-fuels cost-competitive with other transportation fuels, lessen dependence on traditional sources of energy, and reduce greenhouse gas emissions from automobiles; all of which are pivotal societal issues. Spark-ignition engines are equipped with a large number of control actuators to satisfy fuel economy targets and maintain regulated emissions compliance. The increased control flexibility also allows for adaptability to a wide range of fuel compositions, while maintaining efficient operation when input fuel is altered. Ignition timing control is of particular interest because it is the last control parameter prior to the combustion event, and significantly influences engine efficiency and emissions. Although Map-based ignition timing control and calibration routines are state of art, they become cumbersome when the number of control degrees of freedom increases are used in the engine. The increased system complexity motivates the use of model-based methods to minimize product development time and ensure calibration flexibility when the engine is altered during the design process. A closed loop model based ignition timing control algorithm is formulated with: 1) a feed forward fuel type sensitive combustion model to predict combustion duration from spark to 50% mass burned; 2) two virtual fuel property observers for octane number and laminar flame speed feedback; 3) an adaptive combustion phasing target model that is able to self-calibrate for wide range of fuel sources input. The proposed closed loop algorithm is experimentally validated in real time on the dynamometer. Satisfactory results are observed and conclusions are made that the closed loop approach is able to regulate combustion phasing for multi fuel adaptive SI engines

    Low-Pressure EGR in Spark-Ignition Engines: Combustion Effects, System Optimization, Transients & Estimation Algorithms

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    Low-displacement turbocharged spark-ignition engines have become the dominant choice of auto makers in the effort to meet the increasingly stringent emission regulations and fuel efficiency targets. Low-Pressure cooled Exhaust Gas Recirculation introduces important efficiency benefits and complements the shortcomings of highly boosted engines. The main drawback of these configurations is the long air-path which may cause over-dilution limitations during transient operation. The pulsating exhaust environment and the low available pressure differential to drive the recirculation impose additional challenges with respect to feed-forward EGR estimation accuracy. For these reasons, these systems are currently implemented through calibration with less-than-optimum EGR dilution in order to ensure stable operation under all conditions. However, this technique introduces efficiency penalties. Aiming to exploit the full potential of this technology, the goal is to address these challenges and allow operation with near-optimum EGR dilution. This study is focused on three major areas regarding the implementation of Low-Pressure EGR systems: Combustion effects, benefits and constraints System optimization and transient operation Estimation and adaptation Results from system optimization show that fuel efficiency benefits range from 2% โ€“ 3% over drive cycles through pumping and heat loss reduction, and up to 16% or more at higher loads through knock mitigation and fuel enrichment elimination. Soot emissions are also significantly reduced with cooled EGR. Regarding the transient challenges, a methodology that correlates experimental data with simulation results is developed to identify over-dilution limitations related to the engineโ€™s dilution tolerance. Different strategies are proposed to mitigate these issues, including a Neural Network-actuated VVT that controls the internal residual and increases the over-dilution tolerance by 3% of absolute EGR. Physics-based estimation algorithms are also developed, including an exhaust pressure/temperature model which is validated through real-time transient experiments and eliminates the need for exhaust sensors. Furthermore, the installation of an intake oxygen sensor is investigated and an adaptation algorithm based on an Extended Kalman Filter is created. This algorithm delivers short-term and long-term corrections to feed-forward EGR models achieving a final estimation error of less than 1%. The combination of the proposed methodologies, strategies and algorithms allows the implementation of near-optimum EGR dilution and translates to fuel efficiency benefits ranging from 1% at low-load up to 10% at high-load operation over the current state-of-the-art
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