85 research outputs found

    STUDY OF DROPLETS INTERACTIONS ON SOLID SURFACE FOR MANUFACTURING APPLICATIONS

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    Droplet impact behaviors on a solid substrate is a complicated process that involves multiple phenomena on a small scale within a short time. This phenomenon has wide applications in the industrial, medical, and scientific fields. To understand the complicated mechanism, we select the oscillation process as the marked phase to observe and analyze the dynamical balancing between different forces and conservation of energies and compare it to the typical damped harmonic oscillator (DHO) model to examine the character of variables as viscosity, surface tension, and wettability. From the testing results, we created a precise model for post-impact dynamics and described how the solid wettability (which is demonstrated as the contact angle) and the surface tension (which is presented as the weber number) helped control the oscillation dynamics; then further studies reveal the influence of weber number on oscillation frequencies and make a capillary pressure related assumption about satellite droplet separated from the main body. Finally, the latest study reveals the viscositiesโ€™ influence on the dynamics. By creating the overall functions of the Weber and Reynolds numbers, we created a model that can represent the oscillation process under a wide range of conditions

    Corrosion of One-Step Superhydrophobic Stainless-Steel Thermal Spray Coatings

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    As most superhydrophobic coatings are made of soft materials, the need for harder, more robust films is evident in applications where erosional degradation is of concern. The work herein describes a methodology to produce superhydrophobic stainless-steel thermal spray coatings using the high-velocity oxygen fuel technique. Due to the use of a kerosene fuel source, a carbon-rich film is formed on the surface of the thermal spray coatings, lowering the surface energy of the high-energy metallic substrates. The thermal spray process generates a hierarchical micro-/sub-micro-structure that is needed to sustain superhydrophobicity. The effect of spray parameters such as particle velocity and temperature on the coatingโ€™s hydrophobicity state was explored, and a high particle velocity was shown to cause superhydrophobic characteristics. The coatings were characterized using scanning electron microscopy, profilometry, X-ray photoelectron spectroscopy, static water contact angle measurements, water droplet roll-off measurements, and water droplet bouncing tests. The corrosion behavior of the coatings was studied using potentiodynamic polarization measurements in order to correlate water repellency with corrosion resistance; however, all coatings demonstrated active corrosion without passivation. This study describes an interesting phenomenon where superhydrophobicity does not guarantee corrosion resistance and discusses alternative applications for such materials

    Manipulating droplet jumping behaviors on hot substrates with surface topography by controlling vapor bubble growth: from vibration to explosion

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    A major challenge in surface science is rapid removal of sessile liquid droplets from a substrate with complex three-dimensional structures. However, our understanding of interfacial phenomena including droplet wetting dynamics and phase changes on engineered surfaces remains elusive, impeding dexterous designs for agile droplet purging. Here we present a surface topography strategy to modulate droplet jumping behaviors on micropillared substrates at moderate superheat of 20-30 {\deg}C. Specifically, sessile droplets usually dwell in the Wenzel state and therefore the micropillar matrix functions as fin array for heat transfer enhancement. By tuning the feature sizes of micropillars, one can adjust the vapor bubble growth at the droplet base from the heat-transfer-controlled mode to the inertia-controlled mode. As opposed to the relatively slow vibration jumping in seconds, the vapor bubble growth in the inertia-controlled mode on tall-micropillared surface leads to droplet out-of-plane jumping in milliseconds. Such rapid droplet detachment stems from the swift Wenzel-to Cassie transition incurred by vapor bubble burst (explosion), during which the bubble expanding velocity can reach as fast as ~4 m/s. Vapor bubble growth in a droplet and bubble-burst-induced droplet jumping have been less explored. This study unveils the underpinning mechanisms of versatile jumping behaviors of boiling droplets from a hot micro-structured surface and opens up further possibilities for the design of engineered surfaces that mitigate potential damage of vapor explosion or alleviate condensate flooding

    Tuning the interaction of droplets with liquid-repellent surfaces: fundamentals and applications

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    2018 Fall.Includes bibliographical references.Liquid-repellent surfaces can be broadly classified as non-textured surfaces (e.g., smooth slippery surfaces on which droplets can slide easily) and textured surfaces (e.g., super-repellent surfaces on which liquid droplets can bead up and roll off easily). The liquid repellency of smooth slippery surfaces can be adjusted by tuning the surface chemistry. The liquid repellency of super-repellent surfaces can be adjusted by tuning the surface chemistry and surface texture. In this work, by systematically tuning the surface chemistry and surface texture and consequently the surface wettability of solid surfaces, the interaction of droplets of various liquids on liquid-repellent surfaces has been investigated. Based on this understanding, the following phenomena/applications have been investigated/developed: (i New methodology to sort liquid droplets based on their surface tension: By tuning the surface chemistry and surface texture of solid surfaces, we tuned the mobility of liquids with different surface tension on super-repellent surfaces. Utilizing this, we fabricated a simple device with precisely tailored domains of surface chemistry that can sort droplets by surface tension. (ii) New approach to detect the quality of fuel blends: By tuning the surface chemistry of solid surfaces, we investigated the interaction of fuel blends with liquid-repellent surfaces. Based on the understanding gained, we fabricated a simple, field-deployable, low-cost device to rapidly detect the quality of fuel blends by sensing their surface tension with significantly improved resolution. (iii) Novel materials with improved hemocompatibility: By systematically tuning the surface chemistry and surface texture and consequently the surface wettability of solid surfaces, we investigated the interaction of blood with super-repellent surfaces. Based on the understanding gained, we fabricated super-repellent surfaces with enhanced hemocompatibility. (iv) Advanced understanding of droplet splitting upon impacting a macroscopic ridge: By systematically tuning the ridge geometry, we investigated the interaction of impacting water droplets with super-repellent ridges. Based on the understanding gained, we demonstrated the scaling law for predicting the height from which water droplets should fall under gravity onto a super-repellent ridge for them to split into two smaller droplets

    A coating-free superhydrophobic sensing material for full-range human motion and microliter droplet impact detection

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    Traditional waterproofing strategies (e.g. plastic seals, superhydrophobic coatings) of strain sensors greatly limit their sensing performance (e.g., sensitivity, working-range, and working-life). Here a unique ultra-stretchable, coating-free superhydrophobic material is developed for high-performence strain sensing in harsh environments. This material integrates high sensitivity (GF of 2.1 to 214), wide sensing range (up to 447% strain), low resolution (<0.2% strain), dynamic durability (over 10,000 stretching cycles at 50% strain), and ultra-robust superhydrophobicity (mechanically, chemically, thermally, and UV impervious) in a single system, outperforming most of reported waterproof sensors. Such remarkable sensing materials can detect full range human movement, pulse rate and vocal fold vibration. The sensing material is designed to be superhydrophobic throughout its bulk material for work in harsh environments (water, corrosive liquid, high humidity, etc.). More importantly, the superhydrophobicity enables the highly sensitive sensor to detect microliter droplets impact with minimized energy loss. Thus, this sensing material should find many potential applications in wearable electronics, measurement platform, rainfall monitoring and intelligent irrigation system

    Drop Impact on a Solid Surface

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    International audienceA drop hitting a solid surface can deposit, bounce, or splash. Splashing arises from the breakup of a fine liquid sheet that is ejected radially along the sub-strate. Bouncing and deposition depend crucially on the wetting properties of the substrate. In this review, we focus on recent experimental and theoretical studies, which aim at unraveling the underlying physics, characterized by the delicate interplay of not only liquid inertia, viscosity, and surface tension , but also the surrounding gas. The gas cushions the initial contact; it is entrapped in a central microbubble on the substrate; and it promotes the so-called corona splash, by lifting the lamella away from the solid. Particular attention is paid to the influence of surface roughness, natural or engineered to enhance repellency, relevant in many applications. 36

    Developing Superhydrophobic Coatings for Mitigating Aircraft Icing using Plasma Spray Processes

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    In-flight icing due to the presence of super-cooled water droplets is a major problem for aircraft operators. Accumulation of ice on the surface of wings, control parts and sensors can result in a range of problems including navigation issues, decreased efficiency, increasing fuel consumption, forced flight delays and cancelation and, if neglected or mismanaged, even fatal flight incidents. A significant potential solution for mitigating the icing problem is the use of superhydrophobic coatings i.e. coating that are extremely water repelling. Superhydrophobic coatings, by repelling the water droplets, can delay and in some cases prevent ice accumulation. Additionally, superhydrophobic coatings can facilitate ice removal by heating or vibration due to their non-stick properties. The superhydrophobicity of a surface is a result of the combination of the surface micro-texture and its surface energy which is determined by the chemistry of the surface. The major challenge facing the use of superhydrophobic coatings is the fact that low surface energy materials are mainly organic, polymeric compounds that suffer from poor durability, and in addition, micro-textured coatings are typically made by complex and expensive techniques. In this work atmospheric plasma spray (APS) and suspension plasma spray (SPS) which are flexible, scalable and efficient surface engineering techniques, are employed to develop micro-textured superhydrophobic coatings for anti-icing applications. In this research, APS and SPS TiO2 micro-textured coatings are developed. After treatment by a stearic acid solution in order to lower their surface energy, these coatings demonstrate hydrophobicity and superhydrophobicity to different extents. APS coatings that are produced using 10-80 micron-sized particle feedstock, although highly hydrophobic, lack the extreme water repellency known as water mobility, due to their relatively coarse micro-texture. In the SPS process, submicron-sized TiO2 particles in the form of a suspension are used as feedstock. The SPS coatings typically show superhydrophobicity with water contact angles higher than 150ยฐ. The coatings produced using an ethanol-based suspension demonstrated extreme hydrophobicity and a water droplet impacting on their surface bounces back and detaches from them easily. The parameters influencing the SPS process are further studied and optimized to achieve coatings with hierarchical surface micro-texture i.e. a surface with a primary micron-sized and a secondary submicron-sized micro-texture. After optimization of the process, the SPS TiO2 coatings show extreme superhydrophobicity with water contact angles as high as 170ยฐ, water sliding angles as small as 1.3ยฐ and a contact angle hysteresis as small as 4ยฐ. These superhydrophobic SPS TiO2 coatings demonstrate promising results in terms icing performance and durability

    ํŒจํ„ด์„ ์ด์šฉํ•œ ํ‘œ๋ฉด์ œ์–ด์™€ ๊ทธ ํ™œ์šฉ์— ๋Œ€ํ•œ ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ํ™”ํ•™์ƒ๋ฌผ๊ณตํ•™๋ถ€(์—๋„ˆ์ง€ํ™˜๊ฒฝ ํ™”ํ•™์œตํ•ฉ๊ธฐ์ˆ ์ „๊ณต), 2021. 2. ์ฐจ๊ตญํ—Œ.ํ‘œ๋ฉด์€ ๊ตฌ์กฐ์  ๋˜๋Š” ํ™”ํ•™์  ์„ฑ์งˆ์— ๋”ฐ๋ผ ๊ณ ์œ ์˜ ํŠน์„ฑ์„ ๊ฐ–์œผ๋ฉฐ, ์™ธ๋ถ€์—์„œ ๊ฐ€ํ•ด์ง€๋Š” ํž˜์— ์˜ํ•ด ๋ณ€ํ˜•์ด ์ผ์–ด๋‚˜๊ธฐ๋„ ํ•œ๋‹ค. ํ‘œ๋ฉด์„ ๋‚˜๋…ธ ๋‹จ์œ„๋กœ ๊ด€์ฐฐ ๊ฐ€๋Šฅํ•œ ์ „์žํ˜„๋ฏธ๊ฒฝ ์‹œ์Šคํ…œ์ด ๋ฐœ์ „ํ•จ์— ๋”ฐ๋ผ ํ‘œ๋ฉด์—์„œ ๋ฐœ์ƒํ•˜๋Š” ์œ„์™€ ๊ฐ™์€ ํ˜„์ƒ์— ๋Œ€ํ•œ ์—ฐ๊ตฌ๋Š” ์ง€๋‚œ ์ˆ˜์‹ญ ๋…„๊ฐ„ ํ™œ๋ฐœํ•˜๊ฒŒ ์ง„ํ–‰๋˜์—ˆ๋‹ค. ์—ฐ์žŽ, ์†Œ๊ธˆ์Ÿ์ด ๋“ฑ ์ž์—ฐ๊ณ„์—์„œ ๋ฐœ๊ฒฌ๋œ ๋…ํŠนํ•œ ์„ฑ์งˆ์„ ๋‚˜ํƒ€๋‚ด๋Š” ์ดˆ๋ฐœ์ˆ˜ํ‘œ๋ฉด์€ ๋งˆ์ดํฌ๋กœ ๊ตฌ์กฐ ์œ„์— ๋ฏธ์„ธํ•œ ๋‚˜๋…ธ ๊ตฌ์กฐ๋กœ ์ด๋ฃจ์–ด์ง„ ๊ณ„์ธต ๊ตฌ์กฐ์— ์˜ํ•œ ํŠน์„ฑ์œผ๋กœ ๋‚˜ํƒ€๋‚˜๋Š” ํ˜„์ƒ์ธ ๊ฒƒ์ด ๋ฐํ˜€์ง€๋ฉด์„œ ์ด๋ฅผ ๋ชจ๋ฐฉํ•˜์—ฌ ๊ณตํ•™์ ์œผ๋กœ ์ด์šฉํ•ด๋ณด๊ณ ์ž ํ•˜์˜€๊ณ , ํ‘œ๋ฉด์— ๋ฐœ์ƒํ•˜๋Š” ์ฃผ๋ฆ„, ๊ท ์—ด ๋“ฑ์€ ๊ตฌ์กฐ์  ์‹คํŒจ ํ˜น์€ ํŒŒ์†์œผ๋กœ ๊ฐ„์ฃผ๋˜์–ด ์ด๋ฅผ ์ œ์–ดํ•˜๊ณ ์ž ํ•˜์˜€๋‹ค. ํŒจํ„ฐ๋‹์€ ํ‘œ๋ฉด์—์„œ ๋ฐœ์ƒํ•˜๋Š” ํ˜„์ƒ์„ ์ฒด๊ณ„์ ์œผ๋กœ ์ œ์–ดํ•˜๊ณ  ๋ถ„์„ํ•  ์ˆ˜ ์žˆ๋Š” ํ”Œ๋žซํผ์„ ์ œ๊ณตํ•œ๋‹ค. ํŒจํ„ด์˜ ํฌ๊ธฐ, ์ข…๋ฅ˜, ๊ฐ„๊ฒฉ ๋“ฑ์„ ๋‚˜๋…ธ ๋‹จ์œ„๋กœ ์ž์œ ๋กญ๊ฒŒ ์กฐ์ ˆํ•˜์—ฌ ํ‘œ๋ฉด์˜ ๊ตฌ์กฐ์  ํŠน์„ฑ์„ ์ œ์–ดํ•  ์ˆ˜ ์žˆ๊ธฐ ๋•Œ๋ฌธ์ด๋‹ค. ํ‘œ๋ฉด์— ํŒจํ„ด์„ ์ œ์ž‘ํ•˜๋Š” ๋ฐฉ๋ฒ•์œผ๋กœ๋Š” ๋น›๊ณผ ๋งˆ์Šคํฌ๋ฅผ ์ด์šฉํ•œ ๊ด‘ํ•™ ๋ฆฌ์†Œ๊ทธ๋ž˜ํ”ผ, ํ™”ํ•™์  ํŠน์„ฑ์„ ์ด์šฉํ•œ ์‹๊ฐ, ๊ทธ๋ฆฌ๊ณ  PDMS๋ชฐ๋“œ๋ฅผ ์ด์šฉํ•œ ์†Œํ”„ํŠธ ์ž„ํ”„๋ฆฐํŒ… ๋ฐฉ๋ฒ• ๋“ฑ์ด ์•Œ๋ ค์ ธ ์žˆ๋‹ค. ์ดˆ๋ฐœ์ˆ˜ํ‘œ๋ฉด์€ ์ž๊ฐ€์„ธ์ •์œ ๋ฆฌ, ์ž๊ฐ€์„ธ์ •์ž๋™์ฐจ, ์–ผ์ง€ ์•Š๋Š” ํ‘œ๋ฉด ๋“ฑ๊ณผ ๊ฐ™์ด ์‚ฐ์—…์ ์œผ๋กœ ์ด์šฉ ๊ฐ€์น˜๊ฐ€ ๋ถ€๊ฐ๋˜๋ฉด์„œ ์ด๋ฅผ ๊ตฌํ˜„ํ•˜๊ธฐ ์œ„ํ•ด ๋‹ค์–‘ํ•œ ์—ฐ๊ตฌ๊ฐ€ ์ง„ํ–‰๋˜์—ˆ๋‹ค. ํŠนํžˆ, ๊ณ„์ธต๊ตฌ์กฐ๋ฅผ ์ œ์ž‘ํ•จ์— ์žˆ์–ด ๊ณตํ•™์ ์œผ๋กœ ์ดˆ๋ฐœ์ˆ˜ํ˜„์ƒ์„ ์ฒด๊ณ„์  ๋ถ„์„ํ•˜๊ณ ์ž ํŒจํ„ด์„ ํ™œ์šฉํ•˜๋Š” ๋ฐฉ๋ฒ•์ด ์ ์šฉ๋˜์—ˆ๋‹ค. ํ•˜์ง€๋งŒ, ๋Œ€๋ถ€๋ถ„ ๋ฐœํ‘œ๋œ ์—ฐ๊ตฌ๋Š” ๊ณ„์ธต๊ตฌ์กฐ๋ฅผ ์ œ์ž‘ํ•˜๋Š” ๊ณผ์ •์ด ๋ณต์žกํ•˜์—ฌ ์‚ฐ์—…์ ์œผ๋กœ ์ด์šฉํ•˜๊ธฐ์—๋Š” ํ•œ๊ณ„๊ฐ€ ์žˆ์œผ๋ฉฐ ๋”ฐ๋ผ์„œ, ์ดˆ๋ฐœ์ˆ˜ํ‘œ๋ฉด์„ ๊ฐ„๋‹จํ•˜๊ฒŒ ์ œ์ž‘ํ•˜์—ฌ ์‚ฐ์—…๋ถ„์•ผ์— ์ ์šฉ์‹œํ‚ฌ ์ˆ˜ ์žˆ๋Š” ๋ฐฉ๋ฒ•์— ๋Œ€ํ•œ ์—ฐ๊ตฌ๊ฐ€ ํ•„์š”ํ•œ ๋•Œ์ด๋‹ค. ํ•œํŽธ, ํ‘œ๋ฉด์— ๋‹ค์–‘ํ•œ ํ˜•ํƒœ์˜ ํž˜์ด ๊ฐ€ํ•ด์ง€๋ฉด ์ด๋ฅผ ์™„ํ™”์‹œํ‚ค๊ธฐ ์œ„ํ•ด ๋ณ€ํ˜•์ด ์ผ์–ด๋‚œ๋‹ค. ๊ทธ ์ค‘ ์ธ์žฅ์‘๋ ฅ์— ์˜ํ•ด ๋ฐœ์ƒํ•˜๋Š” ๊ท ์—ดํ˜„์ƒ์€ ๋ถˆ๊ทœ์น™์ ์ด๊ณ  ์‹œ์Šคํ…œ์ด ๋ณต์žกํ•˜๊ธฐ ๋•Œ๋ฌธ์— ์กฐ์ ˆํ•˜๊ธฐ ํž˜๋“ค ๋ฟ๋งŒ ์•„๋‹ˆ๋ผ ๋Œ€๋ถ€๋ถ„ ๊ฒฐ์ ์œผ๋กœ ์—ฌ๊ฒจ์ง€๋ฉด์„œ. ์ด๋ฅผ ๋ฐฉ์ง€ํ•˜๊ณ ์ž ํ•˜๋Š” ์—ฐ๊ตฌ์— ์ง‘์ค‘๋˜์–ด ์™”๋‹ค. ํŠนํžˆ ๊ฐ€๋ญ„ ํ˜„์ƒ๊ณผ ๊ฐ™์ด ์šฉ๋งค๊ฐ€ ์ฆ๋ฐœํ•จ์— ๋”ฐ๋ผ ๋ฐœ์ƒํ•˜๋Š” ๊ท ์—ด์€ ๊ณ ๋ถ„์ž ๋ฐ•๋ง‰์—์„œ ๋ฐœ์ƒํ•˜๋Š” ๊ท ์—ดํ˜„์ƒ๋ณด๋‹ค ๋”์šฑ ๋ณต์žกํ•˜๊ณ  ๋ถˆ๊ท ์ผํ•˜๊ฒŒ ํ˜•์„ฑ๋˜๊ธฐ ๋•Œ๋ฌธ์— ํ˜„์žฌ๊นŒ์ง€ ์ด๋ฅผ ์ œ์–ดํ•˜๋Š” ๋ฐฉ๋ฒ•์— ๋Œ€ํ•œ ์—ฐ๊ตฌ๋Š” ๊ฑฐ์˜ ์ง„ํ–‰๋˜์ง€ ์•Š์•„ ์ด์— ๋Œ€ํ•œ ์—ฐ๊ตฌ๊ฐ€ ํ•„์š”ํ•˜๋‹ค. ๋ณธ ํ•™์œ„๋…ผ๋ฌธ์—์„œ๋Š” ํ‘œ๋ฉด์—์„œ ๋ฐœ์ƒํ•˜๋Š” ํ˜„์ƒ ์ค‘ ํŒจํ„ด์„ ์ ์šฉ ํ•˜์—ฌ์ดˆ๋ฐœ์ˆ˜ ํ‘œ๋ฉด๊ณผ ๊ท ์—ด ์ œ์–ด์— ๊ด€ํ•œ ์ฒด๊ณ„์ ์ธ ์—ฐ๊ตฌ๋ฅผ ์ œ์‹œํ•œ๋‹ค. ์‚ฐ์—…์ ์œผ๋กœ ์ด์šฉ ๊ฐ€๋Šฅํ•œ ์ดˆ๋ฐœ์ˆ˜ํ‘œ๋ฉด์„ ๊ฐ„๋‹จํ•˜๊ฒŒ ์ œ์ž‘ํ•˜๋Š” ๋ฐฉ๋ฒ•์„ ์—ฐ๊ตฌํ•˜์˜€๊ณ , ์ดˆ๋ฐœ์ˆ˜ํ‘œ๋ฉด์— ์„ฑ์งˆ์ด ๋‹ค๋ฅธ ํ™”ํ•™์  ํŒจํ„ด์„ ๊ฐ์ธํ•˜์—ฌ ๋ฌผ๋ฐฉ์šธ ์ถฉ๊ฒฉ ์—ญํ•™์˜ ๊ธฐ๊ณ„์  ์กฐ์ ˆ์— ๋Œ€ํ•œ ์—ฐ๊ตฌ๋ฅผ ํ•˜์˜€๋‹ค. ๋˜ํ•œ ๊ฒฐ์ ์œผ๋กœ ์—ฌ๊ฒจ์กŒ๋˜ ๊ฑด์กฐ ์ฝœ๋กœ์ด๋“œ ๋ฐ•๋ง‰์—์„œ ๋ฐœ์ƒํ•˜๋Š” ๊ท ์—ด ํ˜„์ƒ์„ ํŒจํ„ด์„ ์ด์šฉํ•˜์—ฌ ์ฒด๊ณ„์ ์œผ๋กœ ์ œ์–ดํ•˜์˜€์œผ๋ฉฐ, ๋” ๋‚˜์•„๊ฐ€ ๊ท ์—ด๋กœ ์ƒ์„ฑ๋˜๋Š” ์กฐ๊ฐ์˜ ํฌ๊ธฐ๊นŒ์ง€ ์ž์œ ๋กญ๊ฒŒ ์กฐ์ ˆํ•˜๋Š” ๋ฐฉ๋ฒ•์„ ์ œ์‹œํ•˜์—ฌ ๊ณตํ•™์ ์œผ๋กœ ๊ท ์—ด์„ ์œ ์šฉํ•˜๊ฒŒ ํ™œ์šฉํ•  ์ˆ˜ ์žˆ๋Š” ์—ฐ๊ตฌ๋ฅผ ์ œ์‹œํ•œ๋‹ค. ์ œ 1์žฅ์—์„œ๋Š” ์Šคํ”„๋ ˆ์ด์‹œ์Šคํ…œ์„ ํ™œ์šฉํ•˜์—ฌ ๋Œ€๋Ÿ‰ ๋ฉด์ ์—๋„ ๊ฐ„๋‹จํžˆ ์ดˆ๋ฐœ์ˆ˜ํ‘œ๋ฉด์„ ๊ตฌํ˜„ํ•˜๋Š” ๋ฐฉ๋ฒ•์— ๋Œ€ํ•œ ์—ฐ๊ตฌ๋ฅผ ์ œ์‹œํ•˜์˜€๋‹ค. ์ƒ์˜จ์—์„œ๋„ ๋น ๋ฅธ ๋ฐ˜์‘์„ ์œ ๋„ํ•˜๊ธฐ ์œ„ํ•ด ์—ํญ์‹œ-์‚ฌ์ด์˜ฌ ๋ฐ˜์‘์„ ๋„์ž…ํ•˜์—ฌ ์‹ค๋ฆฌ์นด๋‚˜๋…ธ์ž…์ž์™€ ๋ฐ”์ธ๋”, ์šฉ๋งค๋กœ ์ด๋ฃจ์–ด์ง„ ์ฝœ๋กœ์ด๋“œ ์šฉ์•ก์„ ์ œ์กฐํ•˜๊ณ  ๊ฐ ์š”์†Œ์˜ ๋น„์œจ์ด ์ ‘์ด‰๊ฐ, ํˆฌ๋ช…์„ฑ, ํ‘œ๋ฉด ๊ตฌ์กฐ์— ๋ฏธ์น˜๋Š” ์˜ํ–ฅ์„ ์—ฐ๊ตฌํ•˜์˜€๋‹ค. ๋˜ํ•œ ๋‹ค์–‘ํ•œ ํ‘œ๋ฉด์— ์ ์šฉ์‹œ์ผœ ๋ฒ”์šฉ์ ์ธ ํ‘œ๋ฉด์— ์ดˆ๋ฐœ์ˆ˜ํšจ๊ณผ๋ฅผ ๋‚˜ํƒ€๋‚ด๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€๋‹ค. ์ œ 2์žฅ์—์„œ๋Š” ์ดˆ๋ฐœ์ˆ˜ํ‘œ๋ฉด์— ์นœ์ˆ˜์„ฑ์„ ๊ฐ€์ง„ ๋น„๋Œ€์นญ ํ™”ํ•™์  ํŒจํ„ด์„ ๊ฐ์ธ์‹œ์ผœ ๋ฌผ๋ฐฉ์šธ์˜ ๊ฑฐ๋™์ด ์กฐ์ ˆ ๊ฐ€๋Šฅํ•œ ํ‘œ๋ฉด์„ ์ œ์ž‘ํ•˜์˜€๋‹ค. ๊ผญ์ง€์ ์ด ์žˆ๋Š” ํŒจํ„ด์„ ์„ค๊ณ„ํ•˜์—ฌ ๋ฌผ๋ฐฉ์šธ์ด ํ‘œ๋ฉด์— ์ถฉ๊ฒฉํ•˜๊ณ  ๋‹ค์‹œ ํŠ€์–ด ์˜ค๋ฅผ ๋•Œ, ๊ผญ์ง€์  ๋ฐฉํ–ฅ์œผ๋กœ ํŠ€์–ด ์˜ค๋ฅด๋„๋ก ์œ ๋„ํ•˜์˜€๋‹ค. ํŒจํ„ด์˜ ๊ฐ๋„์™€ ์ถฉ๋Œ ๊ฑฐ๋ฆฌ๋ฅผ ์กฐ์ ˆํ•˜์—ฌ ๋ฐฉํ–ฅ์„ฑ์˜ ์ •๋„์— ์˜ํ–ฅ์„ ์ฃผ๋Š” ์š”์ธ์„ ์ฐพ์•„๋‚ด์—ˆ๊ณ , ์ด๋ฅผ ๊ธฐํ•˜ํ•™์  ์ด๋ก  ๊ฐ’๊ณผ ๋น„๊ตํ•˜์—ฌ ์ฐจ์ด๊ฐ€ ์—†๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€๋‹ค. ์ด์™€ ๊ฐ™์€ ํ‘œ๋ฉด์€ ๋ฌผ๋ฆฌ์  ๊ตฌ์กฐ๊ฐ€ ์—†๋Š” ํ‰ํ‰ํ•œ ํ‘œ๋ฉด์—์„œ๋„ ํ™”ํ•™์  ํŒจํ„ด์— ์˜ํ•ด ๋ฌผ๋ฐฉ์šธ์˜ ๊ฑฐ๋™์ด ์กฐ์ ˆ๋˜์—ˆ๊ณ , ๋‚˜์•„๊ฐ€ ๋ฌผ๋ฐฉ์šธ์„ ๊ผญ์ง€์ ๊ณผ ๊ฐ™์€ ํŠน์ • ์œ„์น˜์— ๋ชจ์„ ์ˆ˜ ์žˆ๋‹ค๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€๋‹ค. ์ œ 3์žฅ์—์„œ๋Š” ์ œ 1์žฅ์—์„œ ํ‘œ๋ฉด์„ ์ œ์ž‘ํ•˜๋Š” ๊ณผ์ •์—์„œ ๋ฐœ์ƒํ•œ ๊ท ์—ด ํ˜„์ƒ์„ ๋งˆ์ดํฌ๋กœํŒจํ„ด์„ ์ด์šฉํ•˜์—ฌ ์ œ์–ดํ•˜๋Š” ๋ฐฉ๋ฒ•์„ ์ œ์‹œํ•˜์˜€๋‹ค. TiO2๋กœ ์ด๋ฃจ์–ด์ง„ ์ฝœ๋กœ์ด๋“œ ํ•„๋ฆ„์— ์†Œํ”„ํŠธ ์ž„ํ”„๋ฆฐํŒ… ๊ธฐ๋ฒ•์„ ์ด์šฉํ•˜์—ฌ ํ”„๋ฆฌ์ฆ˜ ํ˜น์€ ํ”ผ๋ผ๋ฏธ๋“œ ๋งˆ์ดํฌ๋กœํŒจํ„ด์„ ๊ฐ์ธ์‹œํ‚ค๊ณ , ์†Œ๊ฒฐ ๊ณผ์ •์„ ํ†ตํ•ด ํ•„๋ฆ„์˜ ์œ ๊ธฐ๋ฌผ์„ ๋ชจ๋‘ ์ œ๊ฑฐํ•˜๋ฉด ํ•„๋ฆ„์— ๋ถ€ํ”ผ ์ˆ˜์ถ•์ด ๋ฐœ์ƒ๋˜๊ณ  ์ŠคํŠธ๋ ˆ์Šค๋Š” ๊ฐ ํŒจํ„ด์˜ ๊ฐ€์žฅ์ž๋ฆฌ์— ์ง‘์ค‘๋˜๊ณ  ๊ท ์—ด์ด ์ด๊ณณ์— ์ƒ์„ฑ๋˜๋„๋ก ์œ ๋„ํ•˜์˜€๋‹ค. ๊ท ์—ด ์ง‘์ค‘ ํ˜„์ƒ์˜ ์ •๋„๋Š” ํ•„๋ฆ„์˜ ๋‘๊ป˜, ๋‚˜๋…ธ ์ž…์ž์˜ ํฌ๊ธฐ, ๊ฐ€์—ด ์†๋„์— ์˜ํ–ฅ์„ ๋ฐ›๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€๋‹ค. ํŠนํžˆ ํ•„๋ฆ„ ๋‘๊ป˜๋Š” ์ƒ์„ฑ๋˜๋Š” ๊ท ์—ด ์กฐ๊ฐ์˜ ๋ฉด์ ์—๋„ ์˜ํ–ฅ์„ ์ฃผ์—ˆ์œผ๋ฉฐ, ๊ฐ ๊ท ์—ด ์กฐ๊ฐ์€ ์ •์‚ฌ๊ฐํ˜• ํ”ผ๋ผ๋ฏธ๋“œ๋กœ ๊ตฌ์„ฑ๋œ ์žฅ์ ์„ ํ™œ์šฉํ•˜์—ฌ ๋ฉด์ ์„ ์‰ฝ๊ฒŒ ์ •๋Ÿ‰ํ™” ํ•˜์˜€๊ณ , ํ•„๋ฆ„ ๋‘๊ป˜์™€ ๋ฉด์ ์ด ๊ฐ–๋Š” ์Šค์ผ€์ผ๋ง ๊ด€๊ณ„๋ฅผ ํ™•์ธํ•˜์˜€๋‹ค. ์ œ 4์žฅ์—์„œ๋Š” ๊ท ์—ด์„ ์ œ์–ดํ•˜๋Š” ๊ฒƒ์—์„œ ๋” ๋‚˜์•„๊ฐ€ ๊ท ์—ด ์กฐ๊ฐ์˜ ํฌ๊ธฐ๊นŒ์ง€ ์ž์œ ๋กญ๊ฒŒ ์กฐ์ ˆํ•˜์—ฌ ์กฐ๊ฐ์„ ๊ธฐํŒ์—์„œ ๋–ผ์–ด๋‚ด์–ด ๋งˆ์ดํฌ๋กœ ๋ธ”๋ก์„ ๋Œ€๋Ÿ‰์œผ๋กœ ๋งŒ๋“ค ์ˆ˜ ์žˆ๋Š” ํ”Œ๋žซํผ์„ ๊ฐœ๋ฐœํ•˜์˜€๋‹ค. ์„œ๋กœ ๋‹ค๋ฅธ ๋†’์ด๋ฅผ ๊ฐ–๋Š” ๋ผ์ธ ํ˜น์€ ํ•„๋ผ ํŒจํ„ด์ด ์žˆ๋Š” ๊ธฐํŒ์„ ์‚ฌ์šฉํ•˜์—ฌ ๊ธฐํŒ์ด ๊ท ์—ด์— ๋ฏธ์น˜๋Š” ์˜ํ–ฅ์„ ๋ถ„์„ํ•˜์˜€๋‹ค. ์ œ์–ด๋œ ์‚ฌ์ด์ฆˆ์˜ ๊ท ์—ด ์กฐ๊ฐ์€ ๊ธฐํŒ์—์„œ ๋–ผ์–ด๋‚ด์–ด ๋งˆ์ดํฌ๋กœ๋ธ”๋ก์œผ๋กœ ์‚ฌ์šฉํ•  ์ˆ˜ ์žˆ์—ˆ๊ณ , ์ด๋ฅผ ํ™œ์šฉํ•˜๋Š” ๋ฐฉ๋ฒ•์„ ์ œ์‹œํ•˜์˜€๋‹ค. ์ด๋Ÿฌํ•œ ์—ฐ๊ตฌ ๊ฒฐ๊ณผ๋Š” ํŒจํ„ด์„ ํ™œ์šฉํ•˜์—ฌ ํ‘œ๋ฉด์„ ์ œ์–ดํ•  ์ˆ˜ ์žˆ๋Š” ๋ฐฉ๋ฒ•์„ ์ œ์‹œํ•˜๊ณ , ์ด๋ฅผ ํ†ตํ•ด ๊ฒฐ์ ์œผ๋กœ ์—ฌ๊ฒจ์กŒ๋˜ ๊ท ์—ด ํ˜„์ƒ์„ ๊ณตํ•™์ ์œผ๋กœ ์‘์šฉ ๊ฐ€๋Šฅํ•˜๋„๋ก ์˜์—ญ์„ ๋„“ํ˜€ ์ค„ ๊ฒƒ์„ ๊ธฐ๋Œ€ํ•œ๋‹ค.The surface properties are affected by the physical structures or chemical characteristics of the surface. As the electron microscope system advanced to allow observing in nanoscale, the fundamental researches of surface properties conducted last few decades. The superhydrophobic surfaces, which was unique property found in lotus leaf, was revealed due to the effect of hierarchical structure, many researchers try to imitate them. Patterning method was introduced to fabricate hierarchical structure to systematic analysis, however, most researches showed limitations for industrial application due to the complicated process. It was necessary to study how to create supernumerary surfaces by implementing hierarchies in a simple way. Meanwhile, mechanical instabilities such as wrinkles, folds and cracks arise when the surface is subjected to various kind of stresses. Among them, the crack phenomenon caused by tensile stress regarded as defect due to its random generation, research was focus on to prevent them. Especially in the drying colloidal film system, there has been little research on how to control it so far, because it is more complex and unevenly formed than the crack phenomenon occurring in the polymer thin film. Pattering provides a platform for systematically controlling and analyzing these phenomena occurred on surfaces. This is because the structural characteristics of the surface can be controlled by freely adjusting the size, type, and spacing of patterns in nano unit. The patterning methods are known as photo lithography, etching and soft imprinting, etc. This dissertation presents a systematic study of superhydrophobic surface and crack manipulation by applying pattern. A simple method to fabricate hierarchical structure was studied for applying industrial field and mechanical control of drop impact dynamics on patterned surfaces was analyzed. The surface crack in desiccation film was controlled by stress localization effect induced by micropatterns. Furthermore, we controlled the size of crack fragments with substrate effect to fabricate homogeneous microblocks and suggest that crack can be usefully utilized in the engineering field. In Chapter 1, we presented a study on fabricating method to transparent superhydrophobic surfaces in large areas. In order to induce a rapid reaction even at room temperature, epoxy-thiol click reaction was introduced into the binder to manufacture a colloid solution consisting of silica nanoparticles, binders and solvents. We investigated the effect of the proportion of each element on the contact angle, transparency and surface structure. Finally, we suggest the spray coating to applicable on a universal surface to coating with superhydrophobicity. In Chapter 2, an asymmetrical chemical pattern with hydrophilic properties was imprinted on the surface to control droplet after impacting the surface. A pattern with vertex was designed to induce droplets bouncing toward vertex after impacting the surface. By adjusting the angle of the pattern and the impacting distance from the vertex, we find factors that influence the degree of directionality, and compare them with geometric theoretical values. This idea provided the platform to collect the droplets on flat surface without any physical patterns in surface. In Chapter 3, we studied the method of controlling random cracks generated during surface fabrication process in Chapter 1 to well-ordered cracks via micropatterns (prisms and pyramids). Micropatterned films were fabricated by the soft imprinting technique with wet TiO2 nanoparticle pastes, followed by calcination to remove organic components. During the calcination, the volume shrinkage occurred in film and stress was concentrated on the edges of each pattern induced cracks to be produced. The degree of stress localization effect was affected by film thickness, nanoparticle size, and heating rate. In particular, film thickness also affected the area of the crack fragments. Utilizing the advantages of our experimental system, we could use a pyramid as a unit to accurately quantify the area of fragments by simply counting the number of pyramids in isolated cracks to identify the scaling relationship between film thickness and area. In Chapter 4, we developed a platform to fabricate various size of pyramidal microblocks by cracking over patterned surfaces. We studied the substrate effect on control cracks and manipulate the fragmentation of TiO2 microscopic pyramids by cracking on prepatterned substrates that have different depths in the substrate. The homogeneous mesoporous microblocks with multifunctionality and various sizes for versatile applications by detaching them from the substrate. This crack engineering method can be used to economically produce a large number of mesoporous microblocks with tunable sizes and functionalities. We believe these studies suggest the ways to control surface properties by utilizing patterns and can give guide to the new strategies on manipulating cracks in desiccation crack system.Contents Chapter 1. Large-Scale Transparent Hydrophobic Surfaces Fabricated by Spray Coating Formulation 1 1.1. Introduction 1 1.2. Experimental Section 3 1.3. Results and Discussion 5 1.3.1. Design of the One-Step Transparent Superhydrophobic Coating Formulation through Spray Process 5 1.3.2. Development of Rapid Curing Binder System in Ambient Condition through Thiol Epoxy Reaction 7 1.3.3. Effects of the Ratio of Binder and Silica NPs on Surface Morphology and Transparency 10 1.3.4 Demonstrate to the Universal Surface by Spray Coating Formulation 15 1.4. Conclusion 17 Chapter 2. Mono Directional Bouncing of Droplets Impacting on Asymmetric Hydrophilic Patterned Surfaces 18 2.1. Introduction 18 2.2. Experimental Section 20 2.3. Results and Discussion 22 2.3.1. Fabrication of Vertex Hydrophilic Patterns on Hydrophobic Surfaces 22 2.3.2. Drop Impacting on Asymmetric Hydrophilic Patterned Surfaces 24 2.3.3. Mechanical Analysis 29 2.4. Conclusion 33 Chapter 3. Control of Surface Cracks by Stress Localization Induced Micropatterns 34 3.1. Introduction 34 3.2. Experimental Section 36 3.3. Results and Discussion 40 3.3.1. Imprinting Effect on Crack Manipulation by Stress Localization Effect 40 3.3.2. Degree of Stress Localization Effect in Film Thickness 45 3.3.3. Effect of Temperature on Crack Propagation 49 3.3.4. Effect of Particle Size and Heating Rate on Critical Cracking Thickness(CCT) 51 3.3.5. Analysis of Crack Fragment Phenomena above the Critical Film Thickness 54 3.4. Conclusion 64 Chapter 4. Tiled Microblocks Obtained on Crack Template with Substrate Patterns 65 4.1. Introduction 65 4.2. Experimental Section 68 4.3. Results and discussion 71 4.3.1. Crack Manipulation Induced by Substrate Effect 71 4.3.2. Control of the Crack Initiation Tips Depending on the Substrate Effect 80 4.3.3. Fabrication of Size and Porosity Controlled Microblocks 84 4.3.4. Multifunctional TiO2 Microblocks 90 4.4. Conclusion 93 Conclusions 94 Bibliography 97 ๊ตญ๋ฌธ ์ดˆ๋ก 109Docto

    Interactions between liquid jets and soap film

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    The interaction between thin jets of water and soap films have been studied. The experiments conducted for this thesis are the first done on jet - soap film interaction with different liquids in the two components. The results are very different from earlier studies where the same liquid was used for both components. Two behaviors were found for the interaction, depending on the incident angle between the incoming jet and soap film and the We number. For low incident angles the jet is bent by the soap film, making it possible to define an index of refraction for the soap film. The bending of the jet done by the soap film increases rapidly when approaching a We number of zero. For We numbers higher than five the jet passes through the film without changing direction. For high incident angles and low We number (โ‰ค 1) the jet rebounds on the film, in analogy with total reflection in optics. The lifetime of the film is measured for different jet speed leading to the conclusion that there is mass exchange between the jet and film. This makes experiments impossible to perform at We โ‰ฅ 17, corresponding to a speed of 1.2 m/s. At this speed the soap film breaks before measurements can be done.Felicia Ullstad Sรฅphinnor och vattenstrรฅlar Sรฅphinnor รคr ett vรคl studerat fenomen inom fysiken. De studeras som ett skolboksexempel pรฅ tunnskiktsinterferens och anvรคnds mycket ofta fรถr att demonstrera att minimering av ytor. Tunna vรคtskestrรฅlar รคr ocksรฅ ett vรคlutforskat omrรฅde, dรฅ de kan anvรคndas till allt frรฅn bestrutning, i blรคckskrivare till att skรคra i stรฅl. Kombinationen av sรฅphinnor och tunna vรคtskestrรฅlar รคr dรคremot knappt undersรถkt tidigare. Vi har skjutit tunna vattenstrรฅlar med olika fart och vinkel mot sรฅphinnan. I figur 1 demonstreras vad som hรคnder nรคr farten pรฅ vattenstrรฅlen รคndras. Bilderna รคr tagna snett under sรฅphinnan och den inkommande vattenstrรฅlen kan ses svagt genom hinnan tillsammens med en reflekterad bild av den utgรฅende vattenstrรฅlen. Figur finns i supplementary material. Figur 1: A: Vattenstrรฅle som gรฅr igenom sรฅphinnan. B: Lรคngre fart pรฅ vattenstrรฅlen ger en stรถrre utgรฅende vinkel. C: ร„nnu lรคgre vattenfart gรถr att strรฅlen absorberas tillfรคlligt i hinnan. D: Lรคgre fart gรถr att strรฅlen reflekteras mot hinnan De olika fenomen som uppkommer i figur 1 kan fรถrklaras frรคmst med hjรคlp av ytspรคnning, hydrofobicitet och den inkommande strรฅlens hastighet. Nรคr vattenstrรฅlens fart sjunker sรฅ รคr det lรคttare fรถr strรฅlen att interagera med sรฅphinnan. Vid tillrรคckligt lรฅga farter kan strรฅlen inte passera genom hinnan utan fastnar i hinnan eller reflekteras. Reflektionen รคr ett fenomen som inte studerats tidigare och tros bero pรฅ att sรฅphinnans yta รคr hydrofobisk vilket tillรฅter strรฅlen att studsa mot hinnan. Hydrofobiciteten tros รคven vara orsak till varfรถr det kan vara svรฅrt att observera hur vattenstrรฅlen fรฅngas av hinnan. Handledare: Johan Zetterberg Examensarbete 15 hp, vt 2013 Fysiska institutionen, Lunds Universite

    Anti-Icing Properties of Femtosecond Laser Surface Processed Material

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    In this thesis, the use of femtosecond laser surface processing (FLSP) to enhance the anti-icing properties of a commonly used aircraft alloy, Al 7075-O Clad is described. By changing the surface morphology through FLSP and the surface chemistry through siloxane vapor deposition, the wettability of Al 7075-O Clad was altered. Condensation and the subsequent freezing of condensates on FLSP Al 7075-O Clad was studied. Both structure height and surface wettability were shown to play a role in the delay of freezing. Freezing occurred on the FLSP superhydrophilic surface faster than on the unprocessed Al 7075-O Clad surface, however, freezing was delayed for all superhydrophobic FLSP surfaces. Tall structure height FLSP functionalized surfaces delayed freezing time longer than short structure height FLSP functionalized surfaces although all were superhydrophobic. It was shown that FLSP functionalized surfaces were able to delay freezing by up to 530 seconds compared to unprocessed Al 7075-O Clad. Self-propelled condensate jumping on FLSP surfaces occurs during the condensing process. The self-propelled jumping phenomena provides a means to promote anti-icing of materials, especially where jumping drops can be swept away in flow conditions The dynamics of supercooled water droplet impact onto FLSP and unprocessed surfaces was also studied. Imaging of supercooled water droplet interaction dynamics on a solid Al 7075-O Clad cold substrate for a droplet diameter below 160 ยตm is shown for the first time. Results indicate that microscale supercooled water droplets at low velocities will stick and freeze to unprocessed Al 7075-O Clad surfaces, while FLSP surfaces will repel droplets under similar conditions. A method for estimating the cooling of small falling water droplets in an environment of about -16 ยฐC is described. This method gives insights for determining the temperature of supercooled droplets for the range of droplet diameters used in the experimental studies included in this paper. In addition, a way to estimate the nucleation site of a supercooled droplet by extrapolation of dendrite front velocity is provided. Advisor: Dennis Alexande
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