10 research outputs found

    ๋ฐ˜๋ณต์žฌํ•˜ ์‹คํ—˜์„ ํ†ตํ•œ ํ”„๋ฆฌ์บ์ŠคํŠธ ์ฝ˜ํฌ๋ฆฌํŠธ ๋ณด-๊ธฐ๋‘ฅ ์ ‘ํ•ฉ๋ถ€์˜ ๊ฑฐ๋™ ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ(์„์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :๊ฑด์ถ•ํ•™๊ณผ,2006.Maste

    ์ €์† ๋ธ”๋ ˆ์ด๋“œ ์ฝ”ํŒ… ์œ ๋™์˜ ๋ถ„์„ ๋ฐ ๋ชจ๋ธ๋ง

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    ํ•™์œ„๋…ผ๋ฌธ (์„์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ํ™”ํ•™์ƒ๋ฌผ๊ณตํ•™๋ถ€, 2021. 2. ๋‚จ์žฌ์šฑ.Blade coating is one of the simplest methods to apply a uniform thin liquid film on a moving substrate. It is widely used from large-scale production in the paper industry to the laboratory scale for fabricating functional films. For the high-speed operation in the commercial field where the viscous force is dominant in the flow, simple hydrodynamic models without considering the capillary force can explain the system and predict the wet film thickness. However, these models are inadequate to the low-speed blade coating system in the laboratory scale where the capillary force becomes dominant. This thesis aims to investigate non-evaporative low-speed blade coating flows, combining experimental, computational, and theoretical approaches. Firstly, the liquid-gas interface formed behind the blade is simplified into the static cylindrical meniscus confined in a plane wedge with an assumption of negligible viscous force. Then, the menisci are classified into three categories depending on how the critical puddle size is represented when the onset of an inflection point on the meniscus and the transition to a thin film occur. Secondly, we have examined the impact of the capillary and the gravitational force on the low-speed blade coating flows of non-evaporative Newtonian fluids. The gravity-dominant flow for the small gap-to-puddle-height ratio produces a thicker film than half of the blade gap, whereas the capillary-dominant flow makes the film much thinner as the puddle is depleted. We derive a simple viscocapillary model that can describe those phenomena. The model shows reasonable agreement with finite element computations that successfully reproduce the experimental results.๋ธ”๋ ˆ์ด๋“œ ์ฝ”ํŒ…์€ ์›€์ง์ด๋Š” ๊ธฐ์žฌ์— ๊ท ์ผํ•œ ๋‘๊ป˜์˜ ๋ฐ•๋ง‰์„ ๋„ํฌํ•˜๋Š” ๊ฐ„๋‹จํ•œ ๋ฐฉ๋ฒ• ์ค‘ ํ•˜๋‚˜์ด๋‹ค. ๋ธ”๋ ˆ์ด๋“œ ์ฝ”ํŒ…์€ ์ œ์ง€ ์‚ฐ์—…๊ณผ ๊ฐ™์€ ๋Œ€๋Ÿ‰ ์ƒ์‚ฐ ๊ณต์ •์—์„œ๋ถ€ํ„ฐ ๊ธฐ๋Šฅ์„ฑ ํ•„๋ฆ„์„ ์ œ์กฐํ•˜๋Š” ์‹คํ—˜์‹ค ๊ทœ๋ชจ์˜ ๊ณต์ •๊นŒ์ง€ ๋„๋ฆฌ ์‚ฌ์šฉ๋œ๋‹ค. ์œ ๋™์—์„œ ์ ์„ฑ๋ ฅ์ด ์ง€๋ฐฐ์ ์ธ ์ƒ์—… ๊ณ ์† ๊ณต์ •์˜ ๊ฒฝ์šฐ, ๋ชจ์„ธ๊ด€ ํž˜์„ ๊ณ ๋ คํ•˜์ง€ ์•Š์€ ๊ฐ„๋‹จํ•œ ์œ ์ฒด ์—ญํ•™ ๋ชจ๋ธ๋“ค๋กœ ์‹œ์Šคํ…œ์„ ์„ค๋ช…ํ•˜๊ณ  ํ•„๋ฆ„์˜ ์ –์Œ ๋‘๊ป˜๋ฅผ ์˜ˆ์ธกํ•  ์ˆ˜ ์žˆ๋‹ค. ๊ทธ๋Ÿฌ๋‚˜ ์ด๋Ÿฌํ•œ ๋ชจ๋ธ๋“ค์€ ๋ชจ์„ธ๊ด€ ํž˜์ด ์ง€๋ฐฐ์ ์ธ ์‹คํ—˜์‹ค ๊ทœ๋ชจ์˜ ์ €์† ๋ธ”๋ ˆ์ด๋“œ ์ฝ”ํŒ… ์‹œ์Šคํ…œ์—๋Š” ์ ํ•ฉํ•˜์ง€ ์•Š๋‹ค. ์ด ๋…ผ๋ฌธ์€ ์‹คํ—˜, ์ „์‚ฐ๋ชจ์‚ฌ, ๊ทธ๋ฆฌ๊ณ  ์ด๋ก ์  ์ ‘๊ทผ๋ฒ•์„ ๊ฒฐํ•ฉํ•˜์—ฌ ์ฆ๋ฐœ์ด ์—†๋Š” ์ €์† ๋ธ”๋ ˆ์ด๋“œ ์ฝ”ํŒ… ์œ ๋™์„ ๋ถ„์„ํ•˜๋Š” ๊ฒƒ์„ ๋ชฉ์ ์œผ๋กœ ํ•œ๋‹ค. ์ฒซ ๋ฒˆ์งธ๋กœ, ๋ธ”๋ ˆ์ด๋“œ ๋’ค์— ํ˜•์„ฑ๋˜๋Š” ๊ธฐ-์•ก ๊ณ„๋ฉด์€ ์ ์„ฑ๋ ฅ์„ ๋ฌด์‹œํ•  ์ˆ˜ ์žˆ๋‹ค๊ณ  ๊ฐ€์ •ํ•˜์—ฌ ์ฝ”๋„ˆ์— ๊ฐ‡ํžŒ ์ •์ ์ธ ์›ํ†ตํ˜• ๋ฉ”๋‹ˆ์Šค์ปค์Šค๋กœ ๋‹จ์ˆœํ™”๋˜์—ˆ๋‹ค. ๊ทธ๋Ÿฐ ๋‹ค์Œ, ๋ฉ”๋‹ˆ์Šค์ปค์Šค์— ๋ณ€๊ณก์ ์ด ์ฒ˜์Œ ๋ฐœ์ƒํ•˜๊ณ  ํผ๋“ค์ด ๋ฐ•๋ง‰์œผ๋กœ ์ „ํ™˜๋  ๋•Œ์˜ ์ž„๊ณ„ ํผ๋“ค ํฌ๊ธฐ๊ฐ€ ์ด๋ก ์ ์œผ๋กœ ์–ด๋–ป๊ฒŒ ํ‘œํ˜„๋˜๋Š”์ง€์— ๋”ฐ๋ผ ๋ฉ”๋‹ˆ์Šค์ปค์Šค๋ฅผ ์„ธ ๊ฐ€์ง€ ๋ฒ”์ฃผ๋กœ ๋ถ„๋ฅ˜ํ•˜์˜€๋‹ค. ๋‘ ๋ฒˆ์งธ๋กœ, ์ฆ๋ฐœ์ด ์—†๋Š” ๋‰ดํ† ๋‹ˆ์•ˆ ์ฝ”ํŒ…์•ก์„ ์‚ฌ์šฉํ•œ ์ €์† ๋ธ”๋ ˆ์ด๋“œ ์ฝ”ํŒ… ์œ ๋™์—์„œ ๋ชจ์„ธ๊ด€ ํž˜๊ณผ ์ค‘๋ ฅ์˜ ์˜ํ–ฅ์„ ๋ถ„์„ํ•˜์˜€๋‹ค. ํผ๋“ค ๋†’์ด๋ณด๋‹ค ๋ธ”๋ ˆ์ด๋“œ ๊ฐญ์ด ๋งค์šฐ ์ž‘์„ ๋•Œ ์ค‘๋ ฅ์ด ์ง€๋ฐฐ์ ์ธ ํ๋ฆ„์ด ๋ฐœ์ƒํ•˜์—ฌ ๋ธ”๋ ˆ์ด๋“œ ๊ฐญ์˜ ์ ˆ๋ฐ˜๋ณด๋‹ค ๋‘๊บผ์šด ํ•„๋ฆ„์ด ๋งŒ๋“ค์–ด์ง€๋Š” ๋ฐ˜๋ฉด, ์ ์„ฑ๋ ฅ์ด ์šฐ์„ธํ•œ ํ๋ฆ„์œผ๋กœ ์ธํ•ด ํผ๋“ค์ด ๊ณ ๊ฐˆ๋จ์— ๋”ฐ๋ผ ํ•„๋ฆ„์ด ๋งค์šฐ ์–‡์•„์ง„๋‹ค. ์šฐ๋ฆฌ๋Š” ์ด๋Ÿฌํ•œ ํ˜„์ƒ๋“ค์„ ์„ค๋ช…ํ•  ์ˆ˜ ์žˆ๋Š” ๊ฐ„๋‹จํ•œ ๋น„์Šค์ฝ”-์บํ•„๋Ÿฌ๋ฆฌ(viscocapillary) ๋ชจ๋ธ์„ ๋„์ถœํ•˜์˜€๋‹ค. ๋ชจ๋ธ์€ ์‹คํ—˜ ๊ฒฐ๊ณผ๋ฅผ ์„ฑ๊ณต์ ์œผ๋กœ ์žฌํ˜„ํ•˜๋Š” ์œ ํ•œ์š”์†Œ๋ฒ• ๊ณ„์‚ฐ๊ณผ ํ•ฉ๋ฆฌ์ ์œผ๋กœ ์ผ์น˜ํ•˜์˜€๋‹ค.Abstract i Contents iii List of Tables v List of Figures vi 1 Introduction 1 2 Classification of static cylindrical menisci confined in a wedge 3 2.1 Introduction 3 2.2 Mathematical formulation of meniscus 5 2.3 The shape factor and the elastica 9 2.4 Classification of menisci 12 2.5 Conclusion 16 3 Simple viscocapillary model for the low-speed blade coating flows 18 3.1 Introduction 18 3.2 Dimensional analysis 20 3.3 Experimental approach 21 3.3.1 Experimental setup and procedure 21 3.3.2 Experimental results 24 3.4 Computational approach 29 3.4.1 Finite element model 29 3.4.2 Computational results 35 3.5 Viscocapillary model 41 3.5.1 Construction of a simple viscocapillary model 41 3.5.2 Validation of the model 48 3.6 Conclusion 52 4 Final remark 53 Abstract (In Korean) 58Maste
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